enhanced particle diffusion through enzyme …
TRANSCRIPT
The Pennsylvania State University
The Graduate School
Chemistry Department
ENHANCED PARTICLE DIFFUSION THROUGH ENZYME CATALYSIS
AND
SILVER TITANIA NANOMOTORS
A Thesis in
Chemistry
by
Shraddha Vishwas Surve
2010 Shraddha Vishwas Surve
Submitted in Partial Fulfillment
of the Requirements
for the Degree of
Master of Science
December 2010
ii
The thesis of Shraddha Vishwas Surve was reviewed and approved by the following
Ayusman Sen
Distinguished Professor of Chemistry
Thesis Advisor
Tom Mallouk
DuPont Professor of Materials Chemistry and Physics
Christine Keating
Associate Professor of Chemistry
Barbara Garrison
Shapiro Professor of Chemistry
Head of the Department of Chemistry
Signatures are on file in the Graduate School
iii
ABSTRACT
In the first part of this thesis I explore the use of enzymes as catalytic motors in order to
drive nanoparticles The two enzymes on which this thesis focuses are horseradish
peroxidase and glucose oxidase Chapter 2 describes the synthesis of carboxylated
polystyrene-silica Janus particles Horseradish peroxidase is immobilized on the
carboxylated polystyrene half of the Janus particle both with and without a linker
between the enzyme and the Janus particle Diffusion coefficients of these particles are
measured to check for enhanced diffusion In Chapter 3 an enzyme cascade system of
horseradish peroxidase and glucose oxidase has been investigated for predator-prey like
behavior Both the enzymes are immobilized on different polystyrene nanospheres and
motion of the spheres is observed in substrate solution of glucose and oxygen Optical
microscopy experiments and diffusion coefficient measurements are carried out in order
to study the predator-prey behavior of these nanoparticles Chapter 4 describes the second
part of the thesis which involves design and synthesis of Ag-TiO2 particles Autonomous
motion of Ag-TiO2 particles can be observed in the presence of hydrogen peroxide
solution Particle motion and inter-particle interactions can be altered by subjecting the
system to UV light trigger
iv
TABLE OF CONTENTS
LIST OF FIGURES vi
LIST OF TABLES ix
ACKNOWLEDGEMENTS x
Chapter 1 Introduction 1
11 Motion at the nanoscale 2
12 Existing nanomotors Mechanisms and uses 6
Chapter 2 Immobilized enzymes on Janus particles as catalytic motors 9
21 Introduction 9
211 Horseradish peroxidase 13
22 Experimental 14
221 Materials and methods 14
222 Synthesis of Janus particles 15
223 Immobilization of enzymes using EDCNHS coupling method 16
224 Enzyme assay 18
225 Diffusion coefficient measurements using Nanosight LM10 19
23 Results 21
231 Enzyme assay 21
232 Diffusion coefficient measurements 23
24 Discussion 25
Chapter 3 Predator-prey system of enzyme immobilized particles 28
31 Introduction 28
311 Glucose oxidase 31
32 Experimental 32
321 Materials and methods 32
v
322 Optical microscopy experiments 33
323 Diffusion coefficient measurements using Nanosight LM10 33
33 Results 34
331 Optical microscopy 34
332 Diffusion coefficient measurements 37
34 Discussion 39
Chapter 4 Silver-titania nanomotors 42
41 Introduction 42
42 Experimental 43
421 Materials and methods 43
422 Synthesis of silver colloidal particles 44
423 Preparation of silver-titania (Ag-TiO2) particles 45
424 Optical microscopy experiments 46
43 Results and Discussion 47
Chapter 5 Summary and Conclusion 52
References 54
vi
LIST OF FIGURES
Figure 1 1 Reciprocal and Nonreciprocal motion8 5
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing
asymmetrical decomposition of substrate into product 10
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in
a theoretical enzyme 11
Figure 2 3 Horseradish peroxidase 13
Figure 2 4 Reaction catalyzed by horseradish peroxidase 14
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation 16
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on
carboxylated polystyrene particles 17
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker 17
Figure 2 8 Nanosight LM 10 instrumentation 19
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen
during experimentation in Nanosight LM10 (b) NTA screen as the particles
are being analyzed for their diffusion coefficients 20
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL
of HRP ΔAmin = 01716 Unitsmg of free enzyme = 52158 22
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus
particles (~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133 23
vii
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles
without and with 6-aminohexanoic acid linker 25
Figure 3 1 Concept of particle aggregation due to cascade reactions of
immobilized enzymes 30
Figure 3 2 Glucose oxidase 31
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase 31
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of
glucose and TMB A In the initial stages single strands form on the surface
of liquid (5Ox) B Single strands branch out and intertwine to form fan-
shaped structures (50x) C Many such structures form and settle down after
20 minutes (20x) 35
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x) 36
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface
area is available for precipitation of TMB which eventually leads to bigger
fan-shaped structures 39
Figure 3 7 Hypothesis for formation of fan-shaped structures 40
Figure 4 1 Physvis particle tracking software 44
Figure 4 2 FESEM image of Ag-TiO2 particles 46
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors 47
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation 48
viii
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles 48
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in
hydrogen peroxide and DI water 50
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation
when UV is turned on 51
ix
LIST OF TABLES
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus
particles without linker 24
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus
particles in the presence of linker 24
Table 3 1 Observations for formation of fan-shaped structures in enzyme
cascade system in presence of different components 34
Table 3 2 Observations for particle aggregation in enzyme cascade system in
presence and absence of TMB 37
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2 38
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01
M glucose and purged with O2 38
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water 49
x
ACKNOWLEDGEMENTS
I would like to thank my advisor Prof Ayusman Sen for his valuable guidance
throughout my research at Penn State He was not only inspiring and encouraging
regarding work but was also very supportive and understanding about life outside work
I would also like to thank my committee members Prof Tom Mallouk and Prof
Christine Keating for being available when I needed guidance and for providing their
valuable advice
I would like to thank my Mom Dad sister and other family members for being
supportive of my decision to come to United States to pursue my graduate studies and for
always being available to share my excitements and disappointments in graduate life I
cannot thank my friend Mahati Elluru enough for her encouraging talks constructive
criticism and praises genuine caring and the list can go on I would like to thank Ambuj
Sharma and Bhavana Achary for being a major part of my life during graduate school and
for making State College feel like home I would like to thank Samudra Sengupta for
being a good friend and mentor who was always around in lab and outside to provide his
valuable insights I would also like to thank Shakuntala Sundararajan Yiying Hong
Michale Ibele Natallia Kulyba and other Sen group members for their support during
graduate school and for creating an enjoyable working environment in the lab
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
ii
The thesis of Shraddha Vishwas Surve was reviewed and approved by the following
Ayusman Sen
Distinguished Professor of Chemistry
Thesis Advisor
Tom Mallouk
DuPont Professor of Materials Chemistry and Physics
Christine Keating
Associate Professor of Chemistry
Barbara Garrison
Shapiro Professor of Chemistry
Head of the Department of Chemistry
Signatures are on file in the Graduate School
iii
ABSTRACT
In the first part of this thesis I explore the use of enzymes as catalytic motors in order to
drive nanoparticles The two enzymes on which this thesis focuses are horseradish
peroxidase and glucose oxidase Chapter 2 describes the synthesis of carboxylated
polystyrene-silica Janus particles Horseradish peroxidase is immobilized on the
carboxylated polystyrene half of the Janus particle both with and without a linker
between the enzyme and the Janus particle Diffusion coefficients of these particles are
measured to check for enhanced diffusion In Chapter 3 an enzyme cascade system of
horseradish peroxidase and glucose oxidase has been investigated for predator-prey like
behavior Both the enzymes are immobilized on different polystyrene nanospheres and
motion of the spheres is observed in substrate solution of glucose and oxygen Optical
microscopy experiments and diffusion coefficient measurements are carried out in order
to study the predator-prey behavior of these nanoparticles Chapter 4 describes the second
part of the thesis which involves design and synthesis of Ag-TiO2 particles Autonomous
motion of Ag-TiO2 particles can be observed in the presence of hydrogen peroxide
solution Particle motion and inter-particle interactions can be altered by subjecting the
system to UV light trigger
iv
TABLE OF CONTENTS
LIST OF FIGURES vi
LIST OF TABLES ix
ACKNOWLEDGEMENTS x
Chapter 1 Introduction 1
11 Motion at the nanoscale 2
12 Existing nanomotors Mechanisms and uses 6
Chapter 2 Immobilized enzymes on Janus particles as catalytic motors 9
21 Introduction 9
211 Horseradish peroxidase 13
22 Experimental 14
221 Materials and methods 14
222 Synthesis of Janus particles 15
223 Immobilization of enzymes using EDCNHS coupling method 16
224 Enzyme assay 18
225 Diffusion coefficient measurements using Nanosight LM10 19
23 Results 21
231 Enzyme assay 21
232 Diffusion coefficient measurements 23
24 Discussion 25
Chapter 3 Predator-prey system of enzyme immobilized particles 28
31 Introduction 28
311 Glucose oxidase 31
32 Experimental 32
321 Materials and methods 32
v
322 Optical microscopy experiments 33
323 Diffusion coefficient measurements using Nanosight LM10 33
33 Results 34
331 Optical microscopy 34
332 Diffusion coefficient measurements 37
34 Discussion 39
Chapter 4 Silver-titania nanomotors 42
41 Introduction 42
42 Experimental 43
421 Materials and methods 43
422 Synthesis of silver colloidal particles 44
423 Preparation of silver-titania (Ag-TiO2) particles 45
424 Optical microscopy experiments 46
43 Results and Discussion 47
Chapter 5 Summary and Conclusion 52
References 54
vi
LIST OF FIGURES
Figure 1 1 Reciprocal and Nonreciprocal motion8 5
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing
asymmetrical decomposition of substrate into product 10
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in
a theoretical enzyme 11
Figure 2 3 Horseradish peroxidase 13
Figure 2 4 Reaction catalyzed by horseradish peroxidase 14
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation 16
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on
carboxylated polystyrene particles 17
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker 17
Figure 2 8 Nanosight LM 10 instrumentation 19
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen
during experimentation in Nanosight LM10 (b) NTA screen as the particles
are being analyzed for their diffusion coefficients 20
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL
of HRP ΔAmin = 01716 Unitsmg of free enzyme = 52158 22
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus
particles (~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133 23
vii
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles
without and with 6-aminohexanoic acid linker 25
Figure 3 1 Concept of particle aggregation due to cascade reactions of
immobilized enzymes 30
Figure 3 2 Glucose oxidase 31
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase 31
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of
glucose and TMB A In the initial stages single strands form on the surface
of liquid (5Ox) B Single strands branch out and intertwine to form fan-
shaped structures (50x) C Many such structures form and settle down after
20 minutes (20x) 35
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x) 36
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface
area is available for precipitation of TMB which eventually leads to bigger
fan-shaped structures 39
Figure 3 7 Hypothesis for formation of fan-shaped structures 40
Figure 4 1 Physvis particle tracking software 44
Figure 4 2 FESEM image of Ag-TiO2 particles 46
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors 47
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation 48
viii
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles 48
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in
hydrogen peroxide and DI water 50
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation
when UV is turned on 51
ix
LIST OF TABLES
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus
particles without linker 24
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus
particles in the presence of linker 24
Table 3 1 Observations for formation of fan-shaped structures in enzyme
cascade system in presence of different components 34
Table 3 2 Observations for particle aggregation in enzyme cascade system in
presence and absence of TMB 37
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2 38
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01
M glucose and purged with O2 38
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water 49
x
ACKNOWLEDGEMENTS
I would like to thank my advisor Prof Ayusman Sen for his valuable guidance
throughout my research at Penn State He was not only inspiring and encouraging
regarding work but was also very supportive and understanding about life outside work
I would also like to thank my committee members Prof Tom Mallouk and Prof
Christine Keating for being available when I needed guidance and for providing their
valuable advice
I would like to thank my Mom Dad sister and other family members for being
supportive of my decision to come to United States to pursue my graduate studies and for
always being available to share my excitements and disappointments in graduate life I
cannot thank my friend Mahati Elluru enough for her encouraging talks constructive
criticism and praises genuine caring and the list can go on I would like to thank Ambuj
Sharma and Bhavana Achary for being a major part of my life during graduate school and
for making State College feel like home I would like to thank Samudra Sengupta for
being a good friend and mentor who was always around in lab and outside to provide his
valuable insights I would also like to thank Shakuntala Sundararajan Yiying Hong
Michale Ibele Natallia Kulyba and other Sen group members for their support during
graduate school and for creating an enjoyable working environment in the lab
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
iii
ABSTRACT
In the first part of this thesis I explore the use of enzymes as catalytic motors in order to
drive nanoparticles The two enzymes on which this thesis focuses are horseradish
peroxidase and glucose oxidase Chapter 2 describes the synthesis of carboxylated
polystyrene-silica Janus particles Horseradish peroxidase is immobilized on the
carboxylated polystyrene half of the Janus particle both with and without a linker
between the enzyme and the Janus particle Diffusion coefficients of these particles are
measured to check for enhanced diffusion In Chapter 3 an enzyme cascade system of
horseradish peroxidase and glucose oxidase has been investigated for predator-prey like
behavior Both the enzymes are immobilized on different polystyrene nanospheres and
motion of the spheres is observed in substrate solution of glucose and oxygen Optical
microscopy experiments and diffusion coefficient measurements are carried out in order
to study the predator-prey behavior of these nanoparticles Chapter 4 describes the second
part of the thesis which involves design and synthesis of Ag-TiO2 particles Autonomous
motion of Ag-TiO2 particles can be observed in the presence of hydrogen peroxide
solution Particle motion and inter-particle interactions can be altered by subjecting the
system to UV light trigger
iv
TABLE OF CONTENTS
LIST OF FIGURES vi
LIST OF TABLES ix
ACKNOWLEDGEMENTS x
Chapter 1 Introduction 1
11 Motion at the nanoscale 2
12 Existing nanomotors Mechanisms and uses 6
Chapter 2 Immobilized enzymes on Janus particles as catalytic motors 9
21 Introduction 9
211 Horseradish peroxidase 13
22 Experimental 14
221 Materials and methods 14
222 Synthesis of Janus particles 15
223 Immobilization of enzymes using EDCNHS coupling method 16
224 Enzyme assay 18
225 Diffusion coefficient measurements using Nanosight LM10 19
23 Results 21
231 Enzyme assay 21
232 Diffusion coefficient measurements 23
24 Discussion 25
Chapter 3 Predator-prey system of enzyme immobilized particles 28
31 Introduction 28
311 Glucose oxidase 31
32 Experimental 32
321 Materials and methods 32
v
322 Optical microscopy experiments 33
323 Diffusion coefficient measurements using Nanosight LM10 33
33 Results 34
331 Optical microscopy 34
332 Diffusion coefficient measurements 37
34 Discussion 39
Chapter 4 Silver-titania nanomotors 42
41 Introduction 42
42 Experimental 43
421 Materials and methods 43
422 Synthesis of silver colloidal particles 44
423 Preparation of silver-titania (Ag-TiO2) particles 45
424 Optical microscopy experiments 46
43 Results and Discussion 47
Chapter 5 Summary and Conclusion 52
References 54
vi
LIST OF FIGURES
Figure 1 1 Reciprocal and Nonreciprocal motion8 5
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing
asymmetrical decomposition of substrate into product 10
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in
a theoretical enzyme 11
Figure 2 3 Horseradish peroxidase 13
Figure 2 4 Reaction catalyzed by horseradish peroxidase 14
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation 16
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on
carboxylated polystyrene particles 17
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker 17
Figure 2 8 Nanosight LM 10 instrumentation 19
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen
during experimentation in Nanosight LM10 (b) NTA screen as the particles
are being analyzed for their diffusion coefficients 20
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL
of HRP ΔAmin = 01716 Unitsmg of free enzyme = 52158 22
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus
particles (~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133 23
vii
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles
without and with 6-aminohexanoic acid linker 25
Figure 3 1 Concept of particle aggregation due to cascade reactions of
immobilized enzymes 30
Figure 3 2 Glucose oxidase 31
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase 31
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of
glucose and TMB A In the initial stages single strands form on the surface
of liquid (5Ox) B Single strands branch out and intertwine to form fan-
shaped structures (50x) C Many such structures form and settle down after
20 minutes (20x) 35
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x) 36
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface
area is available for precipitation of TMB which eventually leads to bigger
fan-shaped structures 39
Figure 3 7 Hypothesis for formation of fan-shaped structures 40
Figure 4 1 Physvis particle tracking software 44
Figure 4 2 FESEM image of Ag-TiO2 particles 46
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors 47
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation 48
viii
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles 48
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in
hydrogen peroxide and DI water 50
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation
when UV is turned on 51
ix
LIST OF TABLES
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus
particles without linker 24
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus
particles in the presence of linker 24
Table 3 1 Observations for formation of fan-shaped structures in enzyme
cascade system in presence of different components 34
Table 3 2 Observations for particle aggregation in enzyme cascade system in
presence and absence of TMB 37
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2 38
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01
M glucose and purged with O2 38
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water 49
x
ACKNOWLEDGEMENTS
I would like to thank my advisor Prof Ayusman Sen for his valuable guidance
throughout my research at Penn State He was not only inspiring and encouraging
regarding work but was also very supportive and understanding about life outside work
I would also like to thank my committee members Prof Tom Mallouk and Prof
Christine Keating for being available when I needed guidance and for providing their
valuable advice
I would like to thank my Mom Dad sister and other family members for being
supportive of my decision to come to United States to pursue my graduate studies and for
always being available to share my excitements and disappointments in graduate life I
cannot thank my friend Mahati Elluru enough for her encouraging talks constructive
criticism and praises genuine caring and the list can go on I would like to thank Ambuj
Sharma and Bhavana Achary for being a major part of my life during graduate school and
for making State College feel like home I would like to thank Samudra Sengupta for
being a good friend and mentor who was always around in lab and outside to provide his
valuable insights I would also like to thank Shakuntala Sundararajan Yiying Hong
Michale Ibele Natallia Kulyba and other Sen group members for their support during
graduate school and for creating an enjoyable working environment in the lab
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
iv
TABLE OF CONTENTS
LIST OF FIGURES vi
LIST OF TABLES ix
ACKNOWLEDGEMENTS x
Chapter 1 Introduction 1
11 Motion at the nanoscale 2
12 Existing nanomotors Mechanisms and uses 6
Chapter 2 Immobilized enzymes on Janus particles as catalytic motors 9
21 Introduction 9
211 Horseradish peroxidase 13
22 Experimental 14
221 Materials and methods 14
222 Synthesis of Janus particles 15
223 Immobilization of enzymes using EDCNHS coupling method 16
224 Enzyme assay 18
225 Diffusion coefficient measurements using Nanosight LM10 19
23 Results 21
231 Enzyme assay 21
232 Diffusion coefficient measurements 23
24 Discussion 25
Chapter 3 Predator-prey system of enzyme immobilized particles 28
31 Introduction 28
311 Glucose oxidase 31
32 Experimental 32
321 Materials and methods 32
v
322 Optical microscopy experiments 33
323 Diffusion coefficient measurements using Nanosight LM10 33
33 Results 34
331 Optical microscopy 34
332 Diffusion coefficient measurements 37
34 Discussion 39
Chapter 4 Silver-titania nanomotors 42
41 Introduction 42
42 Experimental 43
421 Materials and methods 43
422 Synthesis of silver colloidal particles 44
423 Preparation of silver-titania (Ag-TiO2) particles 45
424 Optical microscopy experiments 46
43 Results and Discussion 47
Chapter 5 Summary and Conclusion 52
References 54
vi
LIST OF FIGURES
Figure 1 1 Reciprocal and Nonreciprocal motion8 5
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing
asymmetrical decomposition of substrate into product 10
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in
a theoretical enzyme 11
Figure 2 3 Horseradish peroxidase 13
Figure 2 4 Reaction catalyzed by horseradish peroxidase 14
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation 16
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on
carboxylated polystyrene particles 17
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker 17
Figure 2 8 Nanosight LM 10 instrumentation 19
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen
during experimentation in Nanosight LM10 (b) NTA screen as the particles
are being analyzed for their diffusion coefficients 20
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL
of HRP ΔAmin = 01716 Unitsmg of free enzyme = 52158 22
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus
particles (~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133 23
vii
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles
without and with 6-aminohexanoic acid linker 25
Figure 3 1 Concept of particle aggregation due to cascade reactions of
immobilized enzymes 30
Figure 3 2 Glucose oxidase 31
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase 31
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of
glucose and TMB A In the initial stages single strands form on the surface
of liquid (5Ox) B Single strands branch out and intertwine to form fan-
shaped structures (50x) C Many such structures form and settle down after
20 minutes (20x) 35
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x) 36
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface
area is available for precipitation of TMB which eventually leads to bigger
fan-shaped structures 39
Figure 3 7 Hypothesis for formation of fan-shaped structures 40
Figure 4 1 Physvis particle tracking software 44
Figure 4 2 FESEM image of Ag-TiO2 particles 46
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors 47
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation 48
viii
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles 48
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in
hydrogen peroxide and DI water 50
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation
when UV is turned on 51
ix
LIST OF TABLES
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus
particles without linker 24
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus
particles in the presence of linker 24
Table 3 1 Observations for formation of fan-shaped structures in enzyme
cascade system in presence of different components 34
Table 3 2 Observations for particle aggregation in enzyme cascade system in
presence and absence of TMB 37
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2 38
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01
M glucose and purged with O2 38
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water 49
x
ACKNOWLEDGEMENTS
I would like to thank my advisor Prof Ayusman Sen for his valuable guidance
throughout my research at Penn State He was not only inspiring and encouraging
regarding work but was also very supportive and understanding about life outside work
I would also like to thank my committee members Prof Tom Mallouk and Prof
Christine Keating for being available when I needed guidance and for providing their
valuable advice
I would like to thank my Mom Dad sister and other family members for being
supportive of my decision to come to United States to pursue my graduate studies and for
always being available to share my excitements and disappointments in graduate life I
cannot thank my friend Mahati Elluru enough for her encouraging talks constructive
criticism and praises genuine caring and the list can go on I would like to thank Ambuj
Sharma and Bhavana Achary for being a major part of my life during graduate school and
for making State College feel like home I would like to thank Samudra Sengupta for
being a good friend and mentor who was always around in lab and outside to provide his
valuable insights I would also like to thank Shakuntala Sundararajan Yiying Hong
Michale Ibele Natallia Kulyba and other Sen group members for their support during
graduate school and for creating an enjoyable working environment in the lab
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
v
322 Optical microscopy experiments 33
323 Diffusion coefficient measurements using Nanosight LM10 33
33 Results 34
331 Optical microscopy 34
332 Diffusion coefficient measurements 37
34 Discussion 39
Chapter 4 Silver-titania nanomotors 42
41 Introduction 42
42 Experimental 43
421 Materials and methods 43
422 Synthesis of silver colloidal particles 44
423 Preparation of silver-titania (Ag-TiO2) particles 45
424 Optical microscopy experiments 46
43 Results and Discussion 47
Chapter 5 Summary and Conclusion 52
References 54
vi
LIST OF FIGURES
Figure 1 1 Reciprocal and Nonreciprocal motion8 5
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing
asymmetrical decomposition of substrate into product 10
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in
a theoretical enzyme 11
Figure 2 3 Horseradish peroxidase 13
Figure 2 4 Reaction catalyzed by horseradish peroxidase 14
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation 16
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on
carboxylated polystyrene particles 17
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker 17
Figure 2 8 Nanosight LM 10 instrumentation 19
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen
during experimentation in Nanosight LM10 (b) NTA screen as the particles
are being analyzed for their diffusion coefficients 20
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL
of HRP ΔAmin = 01716 Unitsmg of free enzyme = 52158 22
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus
particles (~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133 23
vii
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles
without and with 6-aminohexanoic acid linker 25
Figure 3 1 Concept of particle aggregation due to cascade reactions of
immobilized enzymes 30
Figure 3 2 Glucose oxidase 31
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase 31
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of
glucose and TMB A In the initial stages single strands form on the surface
of liquid (5Ox) B Single strands branch out and intertwine to form fan-
shaped structures (50x) C Many such structures form and settle down after
20 minutes (20x) 35
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x) 36
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface
area is available for precipitation of TMB which eventually leads to bigger
fan-shaped structures 39
Figure 3 7 Hypothesis for formation of fan-shaped structures 40
Figure 4 1 Physvis particle tracking software 44
Figure 4 2 FESEM image of Ag-TiO2 particles 46
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors 47
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation 48
viii
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles 48
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in
hydrogen peroxide and DI water 50
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation
when UV is turned on 51
ix
LIST OF TABLES
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus
particles without linker 24
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus
particles in the presence of linker 24
Table 3 1 Observations for formation of fan-shaped structures in enzyme
cascade system in presence of different components 34
Table 3 2 Observations for particle aggregation in enzyme cascade system in
presence and absence of TMB 37
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2 38
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01
M glucose and purged with O2 38
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water 49
x
ACKNOWLEDGEMENTS
I would like to thank my advisor Prof Ayusman Sen for his valuable guidance
throughout my research at Penn State He was not only inspiring and encouraging
regarding work but was also very supportive and understanding about life outside work
I would also like to thank my committee members Prof Tom Mallouk and Prof
Christine Keating for being available when I needed guidance and for providing their
valuable advice
I would like to thank my Mom Dad sister and other family members for being
supportive of my decision to come to United States to pursue my graduate studies and for
always being available to share my excitements and disappointments in graduate life I
cannot thank my friend Mahati Elluru enough for her encouraging talks constructive
criticism and praises genuine caring and the list can go on I would like to thank Ambuj
Sharma and Bhavana Achary for being a major part of my life during graduate school and
for making State College feel like home I would like to thank Samudra Sengupta for
being a good friend and mentor who was always around in lab and outside to provide his
valuable insights I would also like to thank Shakuntala Sundararajan Yiying Hong
Michale Ibele Natallia Kulyba and other Sen group members for their support during
graduate school and for creating an enjoyable working environment in the lab
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
vi
LIST OF FIGURES
Figure 1 1 Reciprocal and Nonreciprocal motion8 5
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing
asymmetrical decomposition of substrate into product 10
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in
a theoretical enzyme 11
Figure 2 3 Horseradish peroxidase 13
Figure 2 4 Reaction catalyzed by horseradish peroxidase 14
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation 16
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on
carboxylated polystyrene particles 17
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker 17
Figure 2 8 Nanosight LM 10 instrumentation 19
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen
during experimentation in Nanosight LM10 (b) NTA screen as the particles
are being analyzed for their diffusion coefficients 20
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL
of HRP ΔAmin = 01716 Unitsmg of free enzyme = 52158 22
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus
particles (~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133 23
vii
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles
without and with 6-aminohexanoic acid linker 25
Figure 3 1 Concept of particle aggregation due to cascade reactions of
immobilized enzymes 30
Figure 3 2 Glucose oxidase 31
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase 31
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of
glucose and TMB A In the initial stages single strands form on the surface
of liquid (5Ox) B Single strands branch out and intertwine to form fan-
shaped structures (50x) C Many such structures form and settle down after
20 minutes (20x) 35
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x) 36
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface
area is available for precipitation of TMB which eventually leads to bigger
fan-shaped structures 39
Figure 3 7 Hypothesis for formation of fan-shaped structures 40
Figure 4 1 Physvis particle tracking software 44
Figure 4 2 FESEM image of Ag-TiO2 particles 46
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors 47
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation 48
viii
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles 48
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in
hydrogen peroxide and DI water 50
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation
when UV is turned on 51
ix
LIST OF TABLES
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus
particles without linker 24
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus
particles in the presence of linker 24
Table 3 1 Observations for formation of fan-shaped structures in enzyme
cascade system in presence of different components 34
Table 3 2 Observations for particle aggregation in enzyme cascade system in
presence and absence of TMB 37
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2 38
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01
M glucose and purged with O2 38
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water 49
x
ACKNOWLEDGEMENTS
I would like to thank my advisor Prof Ayusman Sen for his valuable guidance
throughout my research at Penn State He was not only inspiring and encouraging
regarding work but was also very supportive and understanding about life outside work
I would also like to thank my committee members Prof Tom Mallouk and Prof
Christine Keating for being available when I needed guidance and for providing their
valuable advice
I would like to thank my Mom Dad sister and other family members for being
supportive of my decision to come to United States to pursue my graduate studies and for
always being available to share my excitements and disappointments in graduate life I
cannot thank my friend Mahati Elluru enough for her encouraging talks constructive
criticism and praises genuine caring and the list can go on I would like to thank Ambuj
Sharma and Bhavana Achary for being a major part of my life during graduate school and
for making State College feel like home I would like to thank Samudra Sengupta for
being a good friend and mentor who was always around in lab and outside to provide his
valuable insights I would also like to thank Shakuntala Sundararajan Yiying Hong
Michale Ibele Natallia Kulyba and other Sen group members for their support during
graduate school and for creating an enjoyable working environment in the lab
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
vii
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles
without and with 6-aminohexanoic acid linker 25
Figure 3 1 Concept of particle aggregation due to cascade reactions of
immobilized enzymes 30
Figure 3 2 Glucose oxidase 31
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase 31
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of
glucose and TMB A In the initial stages single strands form on the surface
of liquid (5Ox) B Single strands branch out and intertwine to form fan-
shaped structures (50x) C Many such structures form and settle down after
20 minutes (20x) 35
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x) 36
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface
area is available for precipitation of TMB which eventually leads to bigger
fan-shaped structures 39
Figure 3 7 Hypothesis for formation of fan-shaped structures 40
Figure 4 1 Physvis particle tracking software 44
Figure 4 2 FESEM image of Ag-TiO2 particles 46
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors 47
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation 48
viii
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles 48
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in
hydrogen peroxide and DI water 50
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation
when UV is turned on 51
ix
LIST OF TABLES
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus
particles without linker 24
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus
particles in the presence of linker 24
Table 3 1 Observations for formation of fan-shaped structures in enzyme
cascade system in presence of different components 34
Table 3 2 Observations for particle aggregation in enzyme cascade system in
presence and absence of TMB 37
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2 38
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01
M glucose and purged with O2 38
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water 49
x
ACKNOWLEDGEMENTS
I would like to thank my advisor Prof Ayusman Sen for his valuable guidance
throughout my research at Penn State He was not only inspiring and encouraging
regarding work but was also very supportive and understanding about life outside work
I would also like to thank my committee members Prof Tom Mallouk and Prof
Christine Keating for being available when I needed guidance and for providing their
valuable advice
I would like to thank my Mom Dad sister and other family members for being
supportive of my decision to come to United States to pursue my graduate studies and for
always being available to share my excitements and disappointments in graduate life I
cannot thank my friend Mahati Elluru enough for her encouraging talks constructive
criticism and praises genuine caring and the list can go on I would like to thank Ambuj
Sharma and Bhavana Achary for being a major part of my life during graduate school and
for making State College feel like home I would like to thank Samudra Sengupta for
being a good friend and mentor who was always around in lab and outside to provide his
valuable insights I would also like to thank Shakuntala Sundararajan Yiying Hong
Michale Ibele Natallia Kulyba and other Sen group members for their support during
graduate school and for creating an enjoyable working environment in the lab
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
viii
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles 48
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in
hydrogen peroxide and DI water 50
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation
when UV is turned on 51
ix
LIST OF TABLES
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus
particles without linker 24
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus
particles in the presence of linker 24
Table 3 1 Observations for formation of fan-shaped structures in enzyme
cascade system in presence of different components 34
Table 3 2 Observations for particle aggregation in enzyme cascade system in
presence and absence of TMB 37
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2 38
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01
M glucose and purged with O2 38
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water 49
x
ACKNOWLEDGEMENTS
I would like to thank my advisor Prof Ayusman Sen for his valuable guidance
throughout my research at Penn State He was not only inspiring and encouraging
regarding work but was also very supportive and understanding about life outside work
I would also like to thank my committee members Prof Tom Mallouk and Prof
Christine Keating for being available when I needed guidance and for providing their
valuable advice
I would like to thank my Mom Dad sister and other family members for being
supportive of my decision to come to United States to pursue my graduate studies and for
always being available to share my excitements and disappointments in graduate life I
cannot thank my friend Mahati Elluru enough for her encouraging talks constructive
criticism and praises genuine caring and the list can go on I would like to thank Ambuj
Sharma and Bhavana Achary for being a major part of my life during graduate school and
for making State College feel like home I would like to thank Samudra Sengupta for
being a good friend and mentor who was always around in lab and outside to provide his
valuable insights I would also like to thank Shakuntala Sundararajan Yiying Hong
Michale Ibele Natallia Kulyba and other Sen group members for their support during
graduate school and for creating an enjoyable working environment in the lab
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
ix
LIST OF TABLES
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus
particles without linker 24
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus
particles in the presence of linker 24
Table 3 1 Observations for formation of fan-shaped structures in enzyme
cascade system in presence of different components 34
Table 3 2 Observations for particle aggregation in enzyme cascade system in
presence and absence of TMB 37
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2 38
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01
M glucose and purged with O2 38
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water 49
x
ACKNOWLEDGEMENTS
I would like to thank my advisor Prof Ayusman Sen for his valuable guidance
throughout my research at Penn State He was not only inspiring and encouraging
regarding work but was also very supportive and understanding about life outside work
I would also like to thank my committee members Prof Tom Mallouk and Prof
Christine Keating for being available when I needed guidance and for providing their
valuable advice
I would like to thank my Mom Dad sister and other family members for being
supportive of my decision to come to United States to pursue my graduate studies and for
always being available to share my excitements and disappointments in graduate life I
cannot thank my friend Mahati Elluru enough for her encouraging talks constructive
criticism and praises genuine caring and the list can go on I would like to thank Ambuj
Sharma and Bhavana Achary for being a major part of my life during graduate school and
for making State College feel like home I would like to thank Samudra Sengupta for
being a good friend and mentor who was always around in lab and outside to provide his
valuable insights I would also like to thank Shakuntala Sundararajan Yiying Hong
Michale Ibele Natallia Kulyba and other Sen group members for their support during
graduate school and for creating an enjoyable working environment in the lab
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
x
ACKNOWLEDGEMENTS
I would like to thank my advisor Prof Ayusman Sen for his valuable guidance
throughout my research at Penn State He was not only inspiring and encouraging
regarding work but was also very supportive and understanding about life outside work
I would also like to thank my committee members Prof Tom Mallouk and Prof
Christine Keating for being available when I needed guidance and for providing their
valuable advice
I would like to thank my Mom Dad sister and other family members for being
supportive of my decision to come to United States to pursue my graduate studies and for
always being available to share my excitements and disappointments in graduate life I
cannot thank my friend Mahati Elluru enough for her encouraging talks constructive
criticism and praises genuine caring and the list can go on I would like to thank Ambuj
Sharma and Bhavana Achary for being a major part of my life during graduate school and
for making State College feel like home I would like to thank Samudra Sengupta for
being a good friend and mentor who was always around in lab and outside to provide his
valuable insights I would also like to thank Shakuntala Sundararajan Yiying Hong
Michale Ibele Natallia Kulyba and other Sen group members for their support during
graduate school and for creating an enjoyable working environment in the lab
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
1
Chapter 1
Introduction
Motion at the macroscale has been studied and applied for centuries Invention of the
wheel can be considered as the major step for the beginning of synthetic motors at
macroscale The potential applications of the wheel and other similar motors are still
being explored and seem to have endless possibilities Having said that motion at the
nanoscale is just beginning to get explored and can have similar if not greater
implications in the future This thesis is a part of an attempt to develop nanomotors made
from diverse materials operating in different environments to create a pool of
nanomotors which can be used in the future for specific applications
Some of the nanomotors which have already been developed include the pioneering
work by WFPaxton etal of platinum-gold nanomotors1 showing autonomous motion in
hydrogen peroxide motors made by Golestanian2 consisting of micron sized particles
half coated with Pt and others The mechanisms of motion differ in case of different
motors but all have some basic underlying principles which will be highlighted in the
following section An important point to notice in the above mentioned nanomotors is
that they involve metals or solutions which are not biocompatible This puts a restriction
on the application of such motors This thesis attempts to synthesize enzyme based
nanomotors which will be able to overcome these drawbacks and lead to applications in
biological systems like drug delivery and surgery in human body
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
2
Second part of this thesis consists of synthesis and motion of silver-titania nanomotors
which can move autonomously in hydrogen peroxide solution According to some recent
findings3 colloidal silver and hydrogen peroxide may prove to be an effective
combination for treatment of infections in human body Combination of silver particles
and hydrogen peroxide has been tested for disinfection of drinking water and may hold
promise as a secondary disinfecatant which can provide long lasting residual and biofilm
control that is required in water distribution systems4 Silver-titania nanomotors can open
interesting avenues in such applications
11 Motion at the nanoscale
Motion as we understand at macroscale is significantly different from motion at
micronnanoscale A definite discontinuity exists between the two This can be
emphasized by observing the biological systems surrounding us For example at the size
of a cell which is around 10 μm mixing of large molecules is instantaneous due to
diffusion and there is no need for additional convective mixing which is what we
generally think of when we picture macroscopic mixing For instance while convective
flow driven by the pumping of lungs or the use of gills is essential for transport of oxygen
inside an organism which is larger than 1mm in size such as a lizard or a man small
organisms receive nutrients and oxygen solely through diffusion through their tissues5
These differences in motion can be understood both physically and mathematically
Physically as the size of an object decreases the mass and weight decrease with the third
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
3
power of linear size A large body predominantly has gravitational pull of earth acting on
it due to its large mass and other forces like gravitational effect of surrounding objects are
relatively insignificant As the object gets smaller forces such as molecular attraction and
cohesion become more significant and the relative magnitude of the gravitational pull of
the earth on the object decreases due to reduction in mass5 Thus the forces that need to
be considered to cause motion at the macroscale are different than those at the
microscale
Mathematically the difference in motion at macro- and micro- scales can be explained by
means of a dimensionless number called Reynolds number Reynolds number is the ratio
of inertial forces of a system to its viscous forces As size decreases Reynolds number
decreases and the viscous forces become more dominant For a human swimming in
water Reynolds number is around 104 for goldfish it is around 10
2 whereas for an
organism of 1μm size it is around 10-4
to 10-5
[67]
What this means is that as we scale
down from the size of a goldfish to micron sized organisms the inertial forces become
insignificant and the familiar laws of macroscale motion lose their applicability Equation
11 gives the formula for calculating Reynolds number where ρ is density of the fluid
(kgmsup3) μ is the dynamic viscosity of the fluid (kg(mmiddots)) V is the mean fluid velocity
(ms) and D is diameter of particle (m)
Equation 1 1
To understand the implications of low-Reynolds-number systems we can consider the
motion of a macroscopic and an imaginary microscopic scallop Macroscopic scallop
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
4
moves by opening and closing of its shell Inertial thrust is created when a scallop closes
its shell and the scallop moves forward due to the clapping motion (Figure 1 1) This
however does not hold true at the nanoscale since the inertial forces are relatively
insignificant due to the large viscous forces If a microscopic scallop were to exhibit a
similar clapping motion it will just keep moving forward and backward in an oscillatory
kind of motion and will not experience a net motion This is an example of reciprocal
motion which can linearly move a body at macroscale however fails to cause motion at
the microscale
For motion at microscale nonreciprocal motion is necessary8 Nonreciprocal motion
occurs when the path chosen for going from Position A to Position B is different from the
path chosen to come back from Position B to Position A It can be better understood with
the help of Figure 1 1 which shows the change of shapes for a theoretical object going
from Position A to Position B and then returning to Position A by using a different set of
motions This kind of change can lead to motion at the nanomicron scale
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
5
Another factor which gains importance at nanoscale is the dominance and ubiquity of
Brownian motion13
The trajectory of a linearly propelled nanomotor would be
significantly affected by the continuous collision of randomly moving particles in the
environment These collisions deviate the nanomotor from its linear path and hence this
effect needs to be considered while projecting the path of a nanomotor
Motion at the nanoscale can be powered by different types of mechanisms such as
diffusiophoretic electrophoretic osmophoretic chemophoretic thermophoretic and
others Different types of mechanisms of motions may coexist or act individually to cause
Position A Position B
Figure 1 1 Reciprocal and Nonreciprocal motion8
Reciprocal motion
Nonreciprocal motion
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
6
motion Diffusiophoretic motion of particles is caused due to concentration gradients of
solutes in an electrolytenonelectrolyte solution9 Electrophoresis is the motion of a
particle relative to a fluid under the influence of an electric field10
This occurs as the
particle carries an electric surface charge which is acted upon by an electrostatic
coulombic force of the external electric field Osmophoresis is the motion of a
vesiclefluid particle encapsulated in a semi-permeable membrane towards lower
concentration gradient when it is placed in a solution containing solute concentration
gradient1112
Thus considering the numerous mechanisms of motion known to work at
the nanoscale several suitable options are available for the development of artificial
nanomotors
12 Existing nanomotors Mechanisms and uses
Several nanomotors have been developed in the past decade or so A general principle of
working of these nanomotors is that they function by catalytically decomposing the
dissolved fuel to generate asymmetry at their surface or at their interfacial region thereby
causing propulsion13
The self-electrophoretic bimetallic nanowires developed by
WPaxton and A Sen etal consisted of a 2 μm long rod with one tip made up of Au and
the other tip made up of Pt1 These motors were synthesized by electrodeposition in an
alumina template The rods moved autonomously in a solution of hydrogen peroxide
with platinum end forward Pt oxidizes H2O2 to produce H+ and O2 and Au utilizes H
+ to
reduce H2O2 to water This generates an electron flow through the rod and a proton flow
outside the rod resulting in an electric field around the rod in the solution This electric
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
7
field in solution acts on the unbalanced charges within the nanorodrsquos double layer This
moves the nanorod with respect to the surrounding fuel due to the ion flux that is
generated
Bubble propulsion has been predominantly used as mechanism of motion in the motors
developed by Feringa etal His group developed a micromotor by attaching catalase to a
microparticle and placing the particle in a solution containing hydrogen peroxide This
system allowed the microparticle to move by producing oxygen bubbles from the
decomposition of hydrogen peroxide14
A similar motor was later created by Feringarsquos
group which consisted of glucose oxidase and catalase immobilized on a carbon
nanotube in a substrate solution of hydrogen peroxide Glucose oxidase converted
glucose to H2O2 which was then utilized by catalase to produce water and oxygen
thereby propelling the carbon nanotube15
Another interesting example of a self-propelled motor is the polymerization driven motor
developed by Cameron et al16
It consists of polystyrene beads immobilized with ActA
protein which catalyzes actin polymerization leading to the formation of an actin
filament which resembles the flagella of bacteria This actin polymerization propels the
beads at the speed of 001-015 μms
A theoretical model has been proposed by Nafaji and Golestanian etal which consists
of three spheres linked by rigid rods in one dimension17
The length of the rods can
switch between two specific values Due to the nonreciprocal motion of the rod this
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
8
model can swim in low Reynolds number systems An actual model based on
nonreciprocal motion has been developed by Kim etal in which heart cells have been
linked to an asymmetric polydimethylsiloxane robot As the heart cells beat the
asymmetric structure of the device resembles a walking movement18
Most of the nanomicromotors mentioned above are either metallic or work in
environments not compatible with human body Enzymes being an integral part of the
body can solve this problem by operating in suitable substrates already present in the
body fluids The nonreciprocal conformation changes of the enzyme as well as
diffusiophoresis and electrophoresis can conceivably be used to generate motion in case
of enzyme driven nanomotors such motors will be discussed in detail in the following
chapter
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
9
Chapter 2
Immobilized enzymes on Janus particles as catalytic motors
21 Introduction
Enzymes are widely found in biological systems and act on a large variety of substrates
This can make enzymes an ideal choice for powering nanomotors which need to be
biocompatible Several fluids found in the body can act as substrates to the enzymes For
example dissolved glucose which is abundantly found in the body19
is a susbtrate for
enzyme glucose oxidase Urea which is found in the urinary tract20
is a substrate for
urease Hydrogen peroxide produced by phagocytic cells in the body21
is a substrate for
horseradish peroxidase Having motors driven by enzymes can open possibilities of
targeted drug delivery to these parts of the body containing such substrates
Enzymes have already been used to generate motion of carbon nanotubes by mechanism
of bubble propulsion by Feringa etal15
Two other possible mechanisms which may be
able to power motion of nanoparticles using enzymes are asymmetrical decomposition of
substrates into products leading to self-diffusiophoresis (Figure 2 1) and nonreciprocal
changes in enzyme conformation leading to propulsion (Figure 2 2) As seen in Figure 2
1 enzymes which are immobilized on a Janus particle can breakdown the available
substrate in the solution into products causing asymmetric distribution of solutes in the
surrounding fluid This can lead to movement of particle towards the region of lower
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
10
solute concentration by principle of self-diffusiophoresis Figure 2-2 shows the possible
nonreciprocal changes in the conformation of a theoretical protein which can lead to
motion of the protein22
These nonreciprocal changes in conformation are triggered by the
attachment of substrate molecule and release of product molecules from the enzymersquos
active site
Figure 2 1 Enzyme functionalized Janus particle moves upon catalyzing asymmetrical
decomposition of substrate into product
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
11
Figure 2 2 Schematic showing idealized nonreciprocal conformation changes in a
theoretical enzyme22
Enhanced diffusion of a single enzyme molecule by catalysis in a substrate solution has
been demonstrated23
The diffusion coefficient of a single urease molecule was measured
using fluorescence correlation spectroscopy and it was observed that the diffusion of the
urease molecule increases by 16-28 by varying urea concentrations from 0001 M to 1
M Addition of enzyme inhibitors to the system curbed the enhanced diffusion This
enhanced diffusion has been attributed to the force generated by self-electrophoresis by
the enzyme in substrate solution
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
12
Based on the above facts it might be possible to propel a nanoparticle by asymmetric
distribution of enzymes on its surface thereby leading to self-propulsion of the particles
in substrate solution (Figure 2 1) This propulsion may be due to self-
electrophoresisself-diffusiophoresis andor due to nonreciprocal changes in enzyme
conformations Here we aim to investigate a system consisting of polystyrene particles
half coated with enzyme introduced in a suitable substrate solution The enzyme can be
directly linked to the polystyrene particle or it can be linked through a long spacer
molecule (linker) to provide more degrees of freedom to the enzyme
Several factors need to be considered for choosing enzyme for powering motion at the
nanoscale Some of the important factors are the ratio of kcatKm which denotes the
catalytic efficiency of the enzyme possible substrates stability of enzymessubstrates
ease of immobilization relationship with other enzymes in cascade reactions and
commercial availability of the enzymes The enzyme being used in the present study is
horseradish peroxidase It acts on a molecule of hydrogen peroxide and reduces it while
simultaneously oxidizing another substrate molecule In the absence of alternate
oxidizable substrate HRP can oxidize water and oxygen back to hydrogen peroxide24
thus giving an equilibrium reaction
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
13
211 Horseradish peroxidase
Figure 2 3 Horseradish peroxidase
Horseradish peroxidase belongs to the group of peroxidases which are a group of heme-
containing oxidoreductases that act on peroxide as hydrogen donor25
It is a redox
enzyme which contains a protoheme a complex of trivalent iron with 1358-
tetramethyl-24-divinylporphin-67-dipropionic acid as a prosthetic group It is a 44 kDa
protein which includes 33900 Da polypeptide chain bound with eight oligosaccharide
chains The carbohydrate chains improve the stability of the enzyme by protecting it
against radicals formed in the course of the reaction it catalyzes26
Horseradish
peroxidase is found in horseradish and is used widely in bioanalytical applications such
as ELISA and Western blots It decomposes hydrogen peroxide into water and oxygen
while simultaneously oxidizing another substrate27
The oxidizable substrates can be
chromogenic substrates such as 22rsquo55rsquo-tetramethyl-benzidine (TMB) and 33-
diaminobenzidine (DMB) or chemoluminescent substrates like SuperSignal and ECL
luminal28
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
14
Figure 2 4 Reaction catalyzed by horseradish peroxidase
The functional parameters for horseradish peroxidase include Km of 015 mM and kcat of
790 s-1
at an optimum temperature of 20 ordmC and an optimum pH of 6429
Some of the
inhibitors of HRP are 110-phenanthroline aminotriazole and bromine
22 Experimental
221 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by Field
Emission Scanning Electron Microscopy (FESEM) Peroxidase Type I from
Horseradish N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and hydrogen
peroxide solution 50 wt in water were purchased from Sigma-Aldrich N-
hydroxysuccinimide (NHS) ge 97 was purchased from Fluka All chemicals were of
reagent grade and used without further purification Nanopure deionized water was used
for all experiments and preparation of solutions All measurements were made at room
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
15
temperature (25 oC) unless mentioned otherwise The UV-Visible spectroscopy
measurements were performed using Agilent 8453A diode-array UV-Visible
Spectrophotometer with ChemStation UV-Vis Software Diffusion coefficient
measurements were performed using Nanosight LM10
222 Synthesis of Janus particles
A monolayer of particles was prepared according to the procedure (Figure 2 5) by
Goldenberg L et al30
Glass slides were placed on the bottom of a petridish Water was
put into the petridish so that the entire slide was immersed in water A thin layer of
hexane was added on top of water in the petridish A suspension of microspheres in
ethanol (5 ww) was introduced to the water-hexane interface After the monolayer was
formed the glass slide was lifted up through the monolayer with tweezers The
microsphere-covered glass slides were left to dry overnight at room temperature
Following drying a thin film of silica was evaporated on the glass slides in Semicore
evaporator The spheres were partially coated with 30 nm of silica Particles were
removed from the glass slide by gentle sonication The polystyrene-silica (PS-SiO2)
Janus particles thus obtained were washed in deionized water several times before
further immobilization steps were performed FESEM was used to confirm synthesis of
Janus particles
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
16
Figure 2 5 Preparation of PS-SiO2 Janus particles by evaporation
223 Immobilization of enzymes using EDCNHS coupling method
1-Ethyl-3-[3-dimethylaminopropyl]carbodiimide and N-hydroxysulfosuccinimide
(EDCNHS) coupling procedure was followed for immobilizing horseradish peroxidase
type I on 05 μm PS-SiO2 Janus particles (Figure 2 6) In this process EDC reacts with a
carboxyl groups on the Janus particles to form an amine-reactive O-acylisourea
intermediate If this intermediate does not encounter an amine it can hydrolyze and
regenerate the carboxyl group In the presence of NHS EDC can be used to convert
carboxyl groups to amine-reactive sulfo-NHS esters which are much more stable and do
not readily hydrolyze to regenerate carboxyl groups In the current experiment
immobilization was performed in the presence as well as absence of a long spacer
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
17
molecule (linker) between Janus particles and enzymes The chemical 6-aminohexanoic
acid was used as the linker (Figure 2 7) HRP immobilized PS-SiO2 Janus particles were
stored in deionized water until required for further experiments
Figure 2 6 EDCNHS coupling method for immobilization of enzyme on carboxylated
polystyrene particles
Figure 2 7 Immobilization of enzyme on Janus particles with and without 6-
aminohexanoic acid linker
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
18
224 Enzyme assay
Assay for activity of HRP was performed using a spectrophotometric method which
involved using 4-aminoantipyrene as hydrogen donor3132
The reaction rate was
determined by measuring increase in absorbance at 510 nm resulting from the
decomposition of hydrogen peroxide One unit represents the decomposition of 1 μM of
hydrogen peroxide per minute at 25 degC and pH 70 under the specified conditions
The spectrophotometer was set to the wavelength of 510 nm and temperature of 25 degC
Phenol4-aminoantipyrene solution (14 mL) and 00017 M H2O2 solution (15 mL) were
pipetted into each cuvette The cuvette was incubated for 3-4 mins at 25degC and blank was
established A 01 mL solution of diluted enzyme was added to the above mixture and
absorbance was recorded for 4-5 mins Standard graphs of absorbance versus time were
drawn for known concentration of the free enzyme and compared to that of the
immobilized enzyme on the Janus particles The estimate of the amount of enzyme
present on the Janus particles was deduced from the difference between the quantity of
the free enzyme previously added for immobilization and the amount that was measured
to be in the supernatant after some of the enzyme became attached to the Janus particles
The experiment was carried out in triplicate to assess reproducibility
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
19
The formula used to calculate the activity of enzyme is
where ∆Amin denotes the change in absorbance per minute
225 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficients for HRP immobilized particles were measured using Nanosight
LM 10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis (NTA) 20
software in the presence of 003 H2O2 solution as the substrate and also in the presence
of only deionized water The videos were recorded for 30 seconds at the rate of 30 frames
per second Each experiment was carried out in triplicate to assess reproducibility
Particles
visualization
zone
Microscope with
LM 10 unit
LM 10 unit
Figure 2 8 Nanosight LM 10 instrumentation
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
20
Nanosight LM 10 (Figure 2 8) generates videos of population of moving nanoparticles in
a liquid when illuminated by laser light The particles which pass through the laser beam
path are seen by the instrument as small points of light undergoing Brownian motion
(Figure 2 9a)
The videos are further analyzed by NTA (Nanoparticle tracking analysis) software
(Figure 2 9b) which identifies and tracks each particle independently on a frame-by-
frame basis The software also calculates and subtracts any bulk flow in the system The
mean square displacement is calculated for each particle as long as it is visible If the
particle blinks that is if it disappears momentarily and then reappears on the screen the
software will consider the same particle as two separate ones All analysis data is
exported to the excel files in terms of diffusion coefficients of the tracked particles
B A
Figure 2 9 NTA video analysis (a) Particles as they are seen on the screen during
experimentation in Nanosight LM10 (b) NTA screen as the particles are being analyzed for
their diffusion coefficients
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61
21
23 Results
231 Enzyme assay
The activity of free HRP enzyme reported by Sigma Aldrich is 150 unitsmg However
the activity of HRP upon analysis was found to be 52158 unitsmg which is much lower
than the reported value The activity of HRP was found to be further lowered to 2133
unitsmg when it was immobilized on the PS-SiO2 Janus particles in the presence of a
linker The following formula is used to calculate enzyme activity
where ΔAmin is the change in absorbance per minute
22
Figure 2 10 Graph for the assay of solution of free enzyme containing 05mgL of HRP
ΔAmin = 01716 Unitsmg of free enzyme = 52158
During EDCNHS coupling 04 mg enzyme was added to 1 ml of 025 vv suspension
of Janus particles Thus initial concentration of enzyme in the mixture was 04 mgml
Assuming retained activity of the enzyme in supernatant solution the amount of enzyme
in supernatant was calculated to be 03868 mgml from the assay Amount of enzyme
functionalized on the Janus particles was calculated as the difference between enzyme
previously added for immobilization (04 mgml) and the enzyme present in supernatant
(03868 mgml) and was found to be 00132 mgml Enzyme assay was performed on the
enzyme immobilized Janus particles to estimate the activity of immobilized enzyme
(Figure 2 11) and was found to be 2133 unitsmg
y = 0002x + 00516
0
01
02
03
04
05
06
07
08
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
51
0 n
m
Time (sec)
Assay of free enzyme HRP
23
Figure 2 11 Graph for the assay of of immobilized enzyme on 05 μm Janus particles
(~025 vv) ΔAmin = 01853 Unitsmg of free enzyme = 2133
232 Diffusion coefficient measurements
No significant increase was observed in diffusion coefficient of HRP-immobilized Janus
particles in the presence of H2O2 as the substrate Similar results were obtained for
diffusion coefficient measurement with and without linker moieties bridging the enzymes
and particles(Table 2 1 Table 2 2) Thus the linker did not seem to assist in increasing
the particle diffusion by improving or retaining the activity of the enzyme
y = 00015x + 00953
0
01
02
03
04
05
06
07
0 50 100 150 200 250 300 350 400
Ab
sorb
an
ce
510 n
m
Time (sec)
Assay of HRP immobilized 05 μm Janus particles
24
Table 2 1 Diffusion coefficient measurements of HRP immobilized Janus particles
without linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
1359416 1051777 1308675
Standard deviation 4534801 4122075 4918597
Table 2 2 Diffusion coefficient measurements of HRP immobilized Janus particles in
the presence of linker
HRP immobilized
Janus particles in
003 H2O2
Control - Janus
particles in
003 H2O2
Control - HRP
immobilized Janus
particles in DI water
Diffusion coefficient
(10-10
cm2s)
13838 1339829 1407891
Standard deviation 5644692 5649364 5797218
25
Figure 2 12 Diffusion coefficient measurements of PS-SiO2 Janus particles without and
with 6-aminohexanoic acid linker
24 Discussion
To compare the diffusion coefficients observed during the experiments theoretical
diffusion coefficient was calculated using following equation33
r
kTD altraslation
6 Equation 21
where r is the hydrodynamic radius of particle Dtranslational is translational diffusion
coefficient of the particle T is temperature of the system η is the viscosity of fluid
through which the particles are moving and k is the Boltzmann constant From FE-SEM
images the size of the particles used was determined to be 450 nm For 450 nm diameter
0
20
40
60
80
100
120
140
160
Without linker With linker
Dif
fusio
n c
oeff
icie
nt
(10
-10 c
m2s
)
HRP immobilized 05 μm Janus particles - Diffusion coefficient measurements
HRP immobilized Janus particles in 003 H2O2
Control - Janus particles in 003 H2O2
Control - HRP immobilized Janus particles in DI water
26
particle Dtranslational is equal to 109 μm2s which is comparable to the diffusion
coefficient measured for the enzyme immobilized particles
HRP was found to be active on the Janus particles however the activity of the enzyme
was reduced upon immobilization Lower enzyme activity can be due to the coupling
method used which in this case was EDCNHS covalent binding However EDCNHS
coupling method has been shown to significantly retain the enzyme activity when the
enzyme is immobilized on carboxylated multi-walled carbon nanotubes under appropriate
conditions34
Hence EDCNHS binding method by itself is not believed to be
responsible for reduction of enzyme activity upon immobilization
Direct binding of enzyme to the Janus particle may lead to reduction in the enzyme
activity because of space constraints for the enzyme and difficulty for the passage of
substrate to the active site of the enzyme due to stearic hindrance Hence a linker was
inserted between the enzyme and Janus particle during enzyme immobilization However
inserting a linker between the enzyme and the particle did not lead to enhanced diffusion
of Janus particles or increase in enzyme activity of immobilized enzyme
Lack of enhanced diffusion can be firstly attributed to the reduction in enzyme activity
upon immobilization Enzyme activity may be retained by modifying the conditions
during EDCNHS coupling or changing the binding method altogether The degree of
immobilization of HRP on carboxylated Janus particles can possibly be affected by
several factors such as temperature the concentration of the coupling reagent EDC
27
concentration HRP concentration in solution and incubation time34
Different
combinations of these factors can be tested to find optimum conditions for
immobilization of HRP Alternate binding method can involve thiolation of HRP by the
covalent conjugation of mercaptopropionic acid and then the thiolated HRP can then be
attached on the gold surface of a polystyrene-gold Janus particle35
Thus further
modifications can be made to the system in order to retain enzyme activity on the
immobilized particles and thereby power nanomotors using enzymes
28
Chapter 3
Predator-prey system of enzyme immobilized particles
31 Introduction
Predator-prey systems are widely found in nature and play a major role in biological
processes3637
Predator-prey systems include all the interactions in which one organism
pursues andor consumes another organism One familiar predator-prey system at the
macroscale is that of a tiger chasing and consuming a deer Another not so familiar one
includes Baleen whales which eat millions of microscopic planktons at once38
At the
microscale such kind of interactions can be observed in the case of phagocytes in the
body which are capable of engulfing foreign microorganisms and killing them with a
combination of microbicidal systems39
In the case of cancer the tumor is the prey and
the mature myeloid cells in the body are the predator However the tumor here has a
defense mechanism against the predator in which the tumor produces cytokines which
inhibits the maturation of the myeloid cells and thereby prevents predation40
One similarity that can be observed in all these systems is that the prey possesses some
attribute which is desired by the predator which makes the predator chase the prey A
similar relationship is seen in case of enzymes which are involved in cascade reactions41
In cascade reactions product synthesized by one enzyme is the reactant required by
another enzyme to carry out its own catalytic reaction As such there is a predator-prey
29
kind of dependence between the two enzymes which may cause one enzyme to chase the
other enzyme when placed in suitable substrate solutions However the mechanism
hypothesized for such a system is totally different than the mechanism involved in
biological systems In biological systems such as bacterial chemotaxis or phagocytes
chasing foreign particles in human body complex biochemical reactions are responsible
for the predator-prey behavior42
In the proposed enzyme cascade system there are no
complex biochemical reactions involved The principle hypothesized for predator-prey
behavior of enzyme cascade reactions can be explained as follows Motion of synthetic
motors at nanoscale involves two components translational diffusion and rotational
Brownian diffusion At very short time scales of less than 1Dr where Dr (s-1
) is
rotational Brownian diffusion coefficient the motion of particles is unidirectional For
longer time scales of greater than 1Dr the direction of motion is random giving
poweredactive diffusion43
If the chemical homogeneity is broken that is when there is
higher concentration of a substrate present in one direction of the enzyme the enzyme
might acquire a subtle bias which may lead to a spatial aggregation of the enzymes based
on the substrate concentration gradient The bias can be a result of the relationship
between the speed of enzyme diffusion and substrate concentration where higher
substrate concentration lead to higher enzyme diffusion As a result in an enzyme
cascade system one enzyme will migrate towards higher concentration of substrate
which is present near the other enzyme thus giving rise to a predator-prey behavior
Such enzyme cascades are widely found in signaling networks and metabolic pathways in
living cells and can be used to produce predator-prey like nanomotors systems44
The
30
enzymes being used in the present study are horseradish peroxidase and glucose oxidase
Both enzymes are extremely stable4546
Glucose is the substrate for glucose oxidase
which is widely available and highly stable47
Horseradish peroxidase acts on hydrogen
peroxide It is involved in a cascade reaction with glucose oxidase which produces
hydrogen peroxide by converting glucose into gluconic acid (Figure 3 1)48
Figure 3 1 Concept of particle aggregation due to cascade reactions of immobilized
enzymes
In this experiment glucose oxidase (GOx) and horseradish peroxidase (HRP) were
immobilized on polystyrene carboxylate beads of different sizes using EDCNHS
coupling method Glucose and 3355-Tetramethylbenzidine (TMB) were dissolved
together in water and this solution was used as the substrate solution All the components
were present in a single system in DI water Aggregation of particles and precipitation of
oxidized TMB from the solution was expected to be observed when all these components
were present in such a system
Properties of horseradish peroxidase have been discussed in the previous chapter (Section
211 Horseradish peroxidase)
GOxGOx HRPHRP
Glucose + O2Gluconic acid + H2O2
TMB TMB oxidizedBlue precipitate
H2O
Aggregation
31
311 Glucose oxidase
Figure 3 2 Glucose oxidase
Glucose oxidase (GOx) belongs to the group of oxidoreductases and is also called
glucose aerodehydrogenase49
It is obtained from fungi and has been identified as an
antimicrobial enzyme50
GOx binds to β-D-glucopyranose and catalyzes the oxidation
reaction to from gluconolactone while simultaneously reducing oxygen to hydrogen
peroxide51
GOx has high substrate affinity and specificity high stability and high
turnover number which makes it a suitable biocatalyst for industrial applications52
Figure 3 3 Redox reaction of glucose catalyzed by glucose oxidase53
32
GOx is a glycoprotein with molecular weight of 155 kDa and consists of two identical
polypeptide subunits linked together by a disulfide bond The optimum pH for GOx is
55 though it is stable in a broad pH range of 4 to 7 and can be stored for a long period of
time51
The functional parameters for glucose oxidase include Km of 151 mM and kcat of
337 s-1
at temperature of 20 ordmC and pH of 754
Some of the inhibitors of GOx are 2-
Deoxy-D-glucose adenine nucleotides and NaNO3
32 Experimental
321 Materials and methods
Uniform carboxyl modified polystyrene microspheres 05 microm in diameter were obtained
from Polysciences Inc The size of the purchased microspheres was verified by FESEM
Peroxidase Type I from horseradish glucose oxidase Type II-S from Aspergillus niger
N-(3-dimethyl-aminopropyl)-Nrsquo-ethylcarbodiimide (EDC) and Hydrogen peroxide
solution 50 wt in water were purchased from Sigma-Aldrich N-hydroxysuccinimide
(NHS) was purchased from Fluka D-Glucose (99) was purchased from VWR
International Secure-Seal imaging spacers (9mm diameter) for glass slides were obtained
from Sigma Aldrich All chemicals were of reagent grade and used without further
purification Nanopure deionized water was used for all experiments and preparation of
solutions All measurements were made at room temperature (25 oC) unless mentioned
otherwise The UV-Visible measurements were performed using Agilent 8453A diode-
array UV-Visible Spectrophotometer with ChemStation UV-Vis Software Optical
33
microscopy experiments were performed using Axiovert 200 MAT microscope by Carl
Zeiss Diffusion coefficient measurements were obtained using Nanosight LM10
322 Optical microscopy experiments
The enzyme substrate system was observed under optical microscope to check for
aggregation and precipitation due to cascade reactions Several such systems were
studied Each system in general consisted of GOx and HRP immobilized on different
polystyrene particles The substrate solutions consisted of 01 M glucose and different
concentrations of TMB solution The systems were studied in the presence of all the
constituents and in the absence of glucose GOxHRP and TMB Systems consisting of
different sized HRP immobilized particles in substrate solution of 003 hydrogen
peroxide and TMB were also studied Videos were recorded over a period of 24 hours to
observe changes in the system Each experiment was performed atleast thrice to assess
reproducibility of results
323 Diffusion coefficient measurements using Nanosight LM10
Diffusion coefficient of GOx and HRP immobilized particles were measured using
Nanosight LM10 nanoparticle tracking instrument with Nanoparticle Tracking Analysis
(NTA) 20 software Diffusion coefficients were measured for different systems namely
GOx particles in 01 M glucose and oxygen both GOx and HRP functionalized particles
in 01 M glucose and oxygen along with controls for the individual systems Videos were
34
recorded for 30 seconds at the rate of 30 frames per second Each experiment was carried
out in triplicate to assess reproducibility
33 Results
331 Optical microscopy
According to the enzyme cascade model precipitation of TMB was possible only upon
the interaction of GOx and HRP immobilized particles in presence of appropriate
substrate solution Hence in the first set of experiments precipitation of TMB was used
as an indication of the type of interaction between GOx and HRP immobilized particles
Fan-shaped structures were observed when both HRP and GOx immobilized particles
were present in a substrate solution consisting of glucose and TMB These structures
started forming as a single strand and then branched out and intertwined to form the fan-
shaped structures (Figure 3 4)
Table 3 1 Observations for formation of fan-shaped structures in enzyme cascade
system in presence of different components
GOx HRP Glucose TMB Observation
Yes Yes Yes Yes
Fan-shaped structures observed particles associated with
the fan-shaped structures
No Yes Yes Yes No fan-shaped structures
Yes No Yes Yes No fan-shaped structures
Yes Yes No Yes No fan-shaped structures
Yes Yes Yes No No fan-shaped structures
35
Fan-shaped structures can also be observed in the system consisting of only HRP
immobilized particles in substrate solution of hydrogen peroxide and TMB The size of
the fan-shaped structures depends on the size of the enzyme immobilized particles Free
enzymes show extremely tiny structures which are difficult to view under the optical
microscope
Figure 3 4 Formation of fan-shaped structures when both HRP and GOx
immobilized particles were present in a substrate solution consisting of glucose and
TMB A In the initial stages single strands form on the surface of liquid (5Ox) B
Single strands branch out and intertwine to form fan-shaped structures (50x) C Many
such structures form and settle down after 20 minutes (20x)
A
C
B
36
Experiments were performed in the absence of TMB that is the system consisted of GOx
and HRP immobilized particles in glucose substrate solution In the absence of TMB the
particles were expected to move closer to each other without any precipitation due to the
cascade reaction However there was no conclusive aggregation of particles observed in
the system
Free Enzyme 005 μm HRP - immobilized particle
10 μm HRP - immobilized particle 05 μm HRP - immobilized particle
Figure 3 5 Size dependence of fan-shaped structures on the size of HRP -
immobilized particles (20x)
37
Table 3 2 Observations for particle aggregation in enzyme cascade system in presence
and absence of TMB
Glucose GOx HRP TMB Observation
Present Present Present Present Aggregation and precipitate
Present Present Present Absent No conclusive aggregation
Present Absent Present Present No aggregation or ppt
Absent Present Present Present No aggregation or ppt
Present Present Absent Present No aggregation or ppt
332 Diffusion coefficient measurements
Diffusion coefficients were measured for GOx immobilized particles of 05 μm diameter
in substrate solution of 01 M glucose and oxygen Diffusion coefficients of particles
were also measured for system consisting of GOx and HRP functionalized particles in
glucose and oxygen Each experiment was done in triplicate to assess reproducibility
Nanosight visualization chamber being a closed chamber oxygen was purged into all the
solutions before starting the experiments to ensure sufficient supply of oxygen for
catalytic reaction of GOx
38
Table 3 3 Diffusion coefficients for 05 μm GOx immobilized particles in 01 M
glucose purged with O2
Mean
GOx
particles in
01 M
glucose
Control - GOx
particles in DI
water
Control - GOx
particles in 01 M
glucose without
oxygen purging
Control -
particles in 01
M Glucose
Diffusion
coefficient
(x10-10
cm2s)
13316 12888 13827 13702
Standard
deviation 6307 4926 4424 7468
Table 3 4 Diffusion coefficients for GOx and HRP immobilized particles in 01 M
glucose and purged with O2
Mean
GOx- HRP-
functionalized
particles in 01 M
glucose
Control ndash Gox-
HRP- functionalized
particles in DI water
Control - particles
in 01 M glucose
Diffusion coefficient
(x10-10
cm2s)
13005 14434 13702
Standard deviation 5263 6622 7468
No significant increase was observed in diffusion coefficient of enzyme immobilized
particles in any of the systems
39
34 Discussion
Formation of fan-shaped structures due to patterned deposition of oxidized TMB
indicates some kind of interaction between GOx and HRP immobilized particles Particle
diameter dependence of the size of structures can be explained with a simple model in
Figure 3 6 A larger particle will have a higher surface area as compared to a smaller
particle Hence more enzyme is immobilized on the larger particle As a result higher
quantity of TMB is oxidized and precipitated by the larger particle as compared to the
smaller particle This leads to thicker strands of fan-shaped structures eventually scaling
up the whole system to give bigger fan-shaped structures
The exact reason for the formation of such fan-shaped structures which are dependent on
particle size could not be determined It is hypothesized that hydrogen peroxide andor
Figure 3 6 Model for size dependence of fan-shaped structures on the particle
diameter of enzyme immobilized particles Larger the particle more surface area is
available for precipitation of TMB which eventually leads to bigger fan-shaped
structures
Larger particle Smaller particle
40
TMB gradient in the substrate solution might be responsible for such structures If there
is higher concentration of H2O2 on one side of the particle and assuming an even
concentration distribution of TMB there will be selective precipitation in the direction of
H2O2 When several particles come in the vicinity of higher concentration of H2O2 the
precipitation lines will converge to give fan-shaped structures (Figure 3 7)
Figure 3 7 Hypothesis for formation of fan-shaped structures
In the system consisting of GOx immobilized particles HRP immobilized particles
glucose and TMB it was observed that the fan-shaped structures formed at the liquid-air
interface and eventually settled down to the bottom of the glass slide This makes sense
as oxygen is necessary for the catalytic reaction of conversion of glucose to gluconic acid
and hydrogen peroxide which takes place on the surface of GOx immobilized particle As
a result H2O2 is primarily formed at the liquid-air interface and is then used by HRP for
precipitation of TMB
Following the observations that precipitation of TMB occurs at the surface GOx and
HRP immobilized particles are also expected to interact at the surface in the absence of
TMB Due the cascade reaction it was expected that HRP immobilized particles will be
41
attracted to GOx immobilized particles in appropriate substrate solution Experiments
were carried out to visualize inter-particle interactions at the liquid-air interface
However liquid-air interface not being a stable system to image the precise interaction
of GOx and HRP immobilized particles could not be determined Significant external
disturbances were involved at the interface To enable the cascade reaction in the bulk of
the liquid oxygen was purged into the reaction system before starting the experiment
However this did not lead to significant reaction in the bulk of the liquid and the reaction
prominently took place at the liquid-air interface where the oxygen concentration was
higher
In order to observe the interaction of GOx and HRP immobilized particles better imaging
techniques need to be used to observe diffusion of particles in absence of external
disturbances at the liquid-air interface Large quantity of oxygen needs to be purged into
the system and retained to make the reaction more pronounced in the bulk of the substrate
solution Higher concentration of oxygen in water may also be achieved by using oxygen
enriched water which is commercially available55
Alternatively a different enzyme cascade system may be used which does not require a
gaseous substrate56
For example glycogen synthase synthesizes glycogen from glucose-
1-phosphate and glycogen phosphorylase breaks down glycogen to glucose-1-
phosphate57
This system does not require a gaseous substrate and might be able to
overcome the deficiencies of GOx and HRP enzyme cascade system
42
Chapter 4
Silver-titania nanomotors
41 Introduction
Bimetallic nanowires made of platinum and gold have been developed by WPaxton
etal1 The rods move autonomously in a solution of hydrogen peroxide In the present
study silver-titania (Ag-TiO2) particles are being synthesized and investigated for motion
in presence of hydrogen peroxide and UV light With proper control of conditions and
UV light trigger it can be possible to control the speed and direction of motion of these
nanoparticles
Hydrogen peroxide is produced in the human body by phagocytes as an immune response
to foreign particles and pathogens5859
Also silver nanoparticles have been shown to be
biocompatible and capable of interacting with cells in human body without disrupting
cellular function60
Similarly it has been demonstrated that titania is compatible with
different cells DNA and proteins in human body and does not cause toxic effects Hence
silver-titania nanomotors which swim in hydrogen peroxide may open interesting
avenues in applications like targeted drug delivery in those parts of the body where
hydrogen peroxide is present
43
42 Experimental
421 Materials and methods
Silver nitrate (999995) was purchased from Alfa Aesar Gum arabic was purchased
from MP Biomedicals Hydrogen peroxide solution 50 wt in water and ascorbic acid
were purchased from Sigma-Aldrich Nanopure deionized water was used for all
experiments and preparation of all solutions Secure-Seal imaging spacers (9 mm
diameter) were obtained from Sigma Aldrich All experiments were carried out at room
temperature of 25ordmC unless otherwise mentioned Ag-TiO2 particles were synthesized by
evaporation of titania in Semicore electron beam evaporator Particles were characterized
using field-emission scanning electron microscopy Optical microscopy experiments
were performed using Axiovert 200 MAT microscope by Carl Zeiss Particles were
tracked using Physvis particle tracking software (Figure 4 1) in which the position
information of a particle on screen is stored on a frame by frame basis The data is stored
in a dat file as X and Y co-ordinates of particles tracked on the screen This information
can be converted to diffusion coefficients of the particles by further manipulation using
MathWorks-MATLABreg software
44
Figure 4 1 Physvis particle tracking software
422 Synthesis of silver colloidal particles
Silver particles were synthesized by a nucleationgrowth type reaction developed by
Goya and Matijevic61
and modified by Velikov62
Silver nitrate was used as precursor
metal salt for synthesis of silver particles Solution A was 75 ml of 50 mM AgNO3 and
035 by weight gum arabic Solution B was 75 mL of 100 mM 1-ascorbic acid and
035 by weight gum arabic Solution B was rapidly added to solution A in a 250 mL
reaction flask The reaction flask was covered and particles were stirred for 48 hrs After
48 hours particles were allowed to settle for 2-3 hours in refrigerator and supernatant
was separated from the particles Particles were then rinsed with DI water and centrifuged
thrice to obtain pure silver particles Zeta potential of these particles was reported to be
45
around -50 to -60 mV and the size was around 1μm The size of the particles can be
varied by varying the amounts of ascorbic acid and silver nitrate Using molar ratio of 31
of ascorbic acid silver nitrate can give particles of 200 nm diameter whereas ratio of
151 can give particles of upto 5 μm diameter
423 Preparation of silver-titania (Ag-TiO2) particles
A monolayer of silver particles was prepared according to the procedure by Goldenberg
et al63
Glass slides were placed on the bottom of a petridish Water was put into the
petridish so that the entire slide was immersed in water A thin layer of hexane was then
added on top of water in the petridish A suspension of silver particles in ethanol (5
ww) was slowly introduced to the water-hexane interface in the dish After the
monolayer was formed the glass slide was lifted up through the monolayer with tweezers
The silver particles-covered glass slides were left at room temperature to dry overnight
Following drying a thin film of titania was evaporated on the glass slides in Semicore
evaporator (Figure 2 7) The spheres were partially coated with a 10 nm film of titania
Ag-TiO2 particles were removed from the glass slide by gentle sonication FE-SEM was
used to characterize the particles (Figure 4 2) The thin titania layer was not easily
distinguishable due to roughness of the particles
46
Figure 4 2 FESEM image of Ag-TiO2 particles
424 Optical microscopy experiments
Imaging spacers were placed on a glass slide Suspension of Ag-TiO2 particles was
placed on the glass slide and the particles were allowed to settle Movement of particles
was observed in DI water and videos were recorded at 50x magnification of optical
microscope for 30 sec 05 H2O2 was added to the particle suspension on the slide
Videos were recorded at 50x ranging from 30 sec to 10 min to study the movement of
silver titania particles in hydrogen peroxide solution Particles in both DI water and
hydrogen peroxide were subjected to UV light and videos were recorded to study particle
dynamics in presence of UV radiation Particle tracking was performed using Physvis
particle tracking software Atleast 30 particles in every system were tracked for 10
seconds each Particle tracking data was obtained in terms of X and Y coordinates of
particles on screen This data was manipulated using MathWorks-Matlab software and
graphs of mean square displacement of particles versus time were plotted Diffusion
coefficients of particles were calculated from these graphs
47
43 Results and Discussion
Ag-TiO2 particles demonstrated autonomous motion in the presence of H2O2 No UV
light was required for this motion Motion of the particles was accelerated by addition of
fresh H2O2 to the system When subjected to UV radiation the particles displayed
momentary acceleration for 4-5 seconds
Figure 4 3 Mechanism of motion of Ag-TiO2 nanomotors
In the presence of H2O2 silver part of the Ag-TiO2 particle converts H2O2 to H2O and O2
This may lead to propulsion of the Ag-TiO2 particle due to bubble propulsion andor self-
diffusiophoresis In the presence of UV light additional reaction takes place on the
titania part of Ag-TiO2 particle which increases the velocity of the Ag-TiO2 particles
(Figure 4 4) This UV triggered photoactivity of titania is due to hole-electron separation
caused by photons having energy equal to or greater than the band gap of titania646566
Most of the holes-electrons recombine but a small fraction move to the surface and react
with the available redox species like water and oxygen to form protons (H+) superoxide
(O2-) and hydroxyl (OH) radicals
6566 This may lead to propulsion by diffusiophoresis
as well as electrophoresis
48
Figure 4 4 Silver-titania motors move faster when subjected to UV radiation
In addition to linear motion rotational motion is also observed in several particles and
particle aggregates Aggregation of particles can lead to a net circular propulsive force
which can rotate the aggregate as shown in Figure 4 5
Figure 4 5 Rotation due to particle aggregation of Ag-TiO2 particles
Particle tracking by Physvis software revealed a significant increase in diffusion
coefficient of Ag-TiO2 particles in hydrogen peroxide solution as compared to DI water
49
The Ag-TiO2 particles have a diffusion coefficient of 1491 μm2s in hydrogen peroxide
versus only 180 μm2s in DI water Thus the Ag-TiO2 particles move around more than
10 times their body length per second in hydrogen peroxide (Figure 4 6) When
subjected to UV light the particles experience a significant acceleration in hydrogen
peroxide which lasts only for a short duration of time (4-5 sec) after which the particles
return to their original velocity The diffusion coefficient of the particles during this UV
light trigger is found to be around 5093 μm2s UV light trigger does not have any visible
effect on the Ag-TiO2 particles in DI water
Table 4 1 Translational diffusion coefficients of Ag-TiO2 particles in hydrogen
peroxide and water
Mean 05 H2O2 solution DI water
Diffusion coefficient of Ag-TiO2 (μm2s)
without UV light
1491 180
Diffusion coefficient of Ag-TiO2 (μm2s)
in the presence of UV light
5093 113
50
Figure 4 6 Mean square displacement curves of Ag-TiO2 Janus particles in hydrogen
peroxide and DI water
When higher concentration (~30 vv) of Ag-TiO2 particles in hydrogen peroxide is
subjected to UV radiation the particles exhibit pattern formation (Figure 4 7)
Aggregation of Ag-TiO2 Janus particles is observed when UV light is turned on and the
particles disaggregated when UV light is switched off This can be due to predator-prey
kind of interaction between silver and titania half of the Janus particles in the presence of
UV light Oxygen and water that are produced at the silver end by decomposition of
hydrogen peroxide are used up by titania when subjected to UV radiation This can lead
to attraction between titania and silver parts of neighboring Janus particles causing
aggregation
y = 20373x
y = 59994x
y = 71848x
0
100
200
300
400
500
600
700
800
900
0 2 4 6 8 10 12
Mean
sq
uare
dis
pla
cem
en
t (μ
m2s
)
Time (sec)
Mean square displacement vs Time for Ag-TiO2
particles
05 Hydrogen peroxide and UV05 Hydrogen peroxide
DI Water
51
A UV OFF B UV ON
C UV OFF
Figure 4 7 Higher concentrations of Ag-TiO2 particles showing aggregation when UV
is turned on
52
Chapter 5
Summary and Conclusion
In summary no significant enhancement in diffusion was observed in case of enzyme
immobilized Janus particles in substrate solution Presence of a linker between enzyme
and particle did not increase the diffusion coefficient of particles Alternative enzyme
immobilization methods need to be tested like thiolation of enzyme and subsequent
binding to gold surface of a Janus particle35
or expressing the enzyme with polyhistidine
or avidin tag67
This can result in higher enzyme activity upon immobilization and may
lead to enhanced diffusion of Janus particles
Predator-prey system of GOx and HRP immobilized particles showed some promising
results Aggregation of particles and formation of fan-shaped structures by TMB
oxidation were observed under optical microscope when GOx and HRP immobilized
particles glucose and TMB were present in the system The size of the fan-shaped
structures was dependent on the size of enzyme immobilized particles This can be
indicative of some kind of interaction between the GOx and HRP immobilized particles
No conclusive aggregation of GOx and HRP immobilized particles was observed in
absence of TMB Better imaging techniques are required to study the interaction of GOx
and HRP immobilized particles at the unstable liquid-air interface where majority of the
reaction takes place Other enzyme cascade systems not requiring gaseous reactants like
glycogen synthase and glycogen phosphorylase should be tested for similar activity
53
Ag-TiO2 particles were found to exhibit autonomous motion in the presence of hydrogen
peroxide solution The motion was momentarily accelerated upon exposure to UV
radiation The particles showed a diffusion coefficient of 1491 μm2s in hydrogen
peroxide versus only 180 μm2s in DI water Upon subjecting particles to UV radiation in
presence of H2O2 diffusion coefficient increased to 5093 μm2s for a period of 4-5
seconds In addition to linear motion rotating motion could also be observed in some
particle aggregates Further development of these aggregate structures can lead to
formation of rotors at nanoscale Higher concentration of silver-titania particles in
hydrogen peroxide displayed aggregation in presence of UV light and disaggregated
when UV light was switched off This may be attributed to the predator-prey kind of
interaction between silver and titania where oxygen and water that are produced by
silver by decomposition of hydrogen peroxide are used up by titania when subjected to
UV radiation This promises to be an interesting system and needs to be further
investigated to explore its properties
54
References
1 Paxton WF Sundararajan S Mallouk TE Sen A Angew Chem Int Ed Engl
2006 45 5420-5429
2 Golestanian R Liverpool TB Adjari A Phys Rev Lett 2005 94 220801
3 httpwwwsilvermedicineorgh2o2html
4 Rami Pedahzur Ovadia Lev Badri Fattal Hillel Shuval Water Science and Technology
1995 31(5-6) 123-129
5 W Went F American Scientist 1968 56
6 Adriano Cavalcanti Tad Hogg Bijan Shirinzadeh IEEE MHS 2006 International
Symposium on Micro-NanoMechatronics and Human Science 2006 226-232
7 EM Purcell American Journal of Physics 1977 45 3-11
8 Golestanian R Phys Rev Lett 2010 105 018103(1)-018103(4)
9 S S Dukhin Z R Ulberg G L Dvornichenko B V Deryagin Russian Chemical
Bulletin 1983 31(8) 1535-1544
10 Dukhin AS Goetz PJ Ultrasound for characterizing colloids Particle sizing zeta
potential rheology Elsevier 2002 59
11 HJKeh HJTu Trends in Colloid and Interface Science XIV Progress in Colloid and
Polymer Science 2000 115 174-180
12 D Zinemanas A Nir International Journal of Multiphase Flow 1995 21(5) 787-800
55
13 Stephen Ebbens Jonathan Howse Soft matter 2010 6 726-739
14 J Vicario R Eelkema W R Browne A Meetsma R M La Crois B L Feringa
Chem Commun 2005 31 3936
15 Davide Pantarotto Wesley R Browne Ben L Feringa Chem Commun 2008 1533 -
1535
16 Lisa A Cameron Matthew J Footer Alexander van Oudenaarden Julie A Theriot
PNAS 1999 96(9) 4908-4913
17 Ali Najafi Ramin Golestanian Phys Rev E 2004 69 062901
18 Jinseok Kim Jungyul Park Sungwook Yang Jeongeun Baek Byungkyu Kim Sang
Ho Lee Eui-Sung Yoon Kukjin Chun Sukho Park Lab Chip 2007 7 1504 - 1508
19 Kurt M Dubowski Clinical Chemistry 2008 5411 1919ndash1920
20 Spector DA Yang Q Wade JB Am J Physiol Renal Physiol 2007 292(1) 467-474
21 Rhee SG Chang TS Bae YS Lee SR Kang SW J Am Soc Nephrol 2003 14(8-3)
211-215
22 Sakaue T Kapral R Mikhailov A S Eur Phys J B 2010 75 381ndash387
23 Muddana H S Sengupta S Mallouk T E Sen A Butler P J J Am Chem Soc
2010 132 (7) 2110ndash2111
24 Baker CJ Deahl K Domek J Orlandi EW Arch Biochem Biophys 2000 382(2) 232-
237
25 V Vojinovic RH Carvalho F Lemos JMS Cabral LP Fonseca BS Ferreira
Biochemical Engineering Journal 2007 35 126-135
56
26
OV Lebedeva NN Ugarova Russian Chemical Bulletin 1996 45(1) 18-25
27 Nigel C Veitch Phytochemistry 2004 65(3) 249-259
28 Kenneth H Petersen Journal of Immunological Methods 2009 340(1) 86-89
29 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
30 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
31 httpwwwgoldbiocompdf3761-Protocol201pdf
32 Av Rovisco Pais Lisboa Portugal T amp D Technology West Yorkshire UK Journal
of Molecular Catalysis B Enzymatic 2004 28(2-3) 129-135
33 httpwwwphysicsnyuedugrierlabmethodsnode11html
34 Yoon-Mee Lee1 O-Yul Kwon Yeo-Joon Yoon Keungarp Ryu Biotechnology Letters
2006 28 39ndash43
35 JC Pyun SD Kim JW Chung Analytical Biochemistry 2005 347(2) 227-233
36 George H Pimbley Jr Mathematical Biosciences 1974 20(1-2) 27-51
37 Andy Fenton Sarah E Perkins Parasitology 2010 137 1027-1038
38 Mead James G Brownell Robert L Mammal Species of the World A Taxonomic and
Geographic Reference (3rd ed) Johns Hopkins University Press 2005 2 2142
57
39
Krause KH Schweiz Med Wochenschr 2000 130(4) 97-100
40 Irina Kareva Faina Berezovskaya Carlos Castillo-Chavez Journal of Biological
Dynamics 2010 4(4)315 - 327
41 Delaittre G Reynhout I Cornelissen J Nolte R Chemistry ndash A European Journal
2009 15 12600ndash12603
42 C Buller DH Johnson RC Tschumper Investigative Ophthalmology amp Visual Science
1990 31 2156-2163
43 Robert M Mazo Brownian Motion Fluctuations Dynamics and Applications Oxford
Science Publications 2009 57
44 Vivek K Mutalik KV Venkatesh Theoretical Biology and Medical Modelling 2005 2
19
45 Satoshi Nakamura Kunimasa Koga Biochemical and Biophysical Research
Communications 1977 78(2) 806-810
46 Krishnananda Chattopadhyay Shyamalava Mazumdar Biochemistry 2000 39 (1)
263ndash270
47 Satoshi Nakamura Yasuyuki Ogura J Biochem 1968 63 (3) 308-316
48 van Dongen SF Nallani M Cornelissen JJ Nolte RJ van Hest JC Chemistry 2009
15(5) 1107-1114
49 Ronald Bentley Methods in Enzymology 1955 1 340-345
50 Vartiainen J Raumlttouml M Paulussen S Packaging Technology and Science 2005
18 243ndash251
58
51 GA Sherbeny AA Shindia YMMM Sheriff International Journal of Agriculture
and Biology 2005 7
52 D Rando G-W Kohring F Giffhorn Appl Microbiol Biotechnol 1997 48
53 Worthington enzyme manual Worthington Biochemical Corporation
httpworthington-biochemcomgopdefaulthtml
54 httpwwwbrenda-enzymesorgphpresult_flatphp4ecno=11117
55 httpwwwoxygenphwatercom
56 P Boon Chock Sue Goo Rhee and Earl R Stadtman Annu Rev Biochem 1980 49
813-841
57 Sybil Golden P A Wals Joseph Katz Analytical Biochemistry 1977 77(2) 436-445
58 R L Baehner S K Murrmann J Davis R B Johnston Jr J Clin Invest 1975 56(3)
571ndash576
59 I Bejarano M P Terroacuten S D Paredes C Barriga A B Rodriacuteguez J A Pariente
Molecular and Cellular Biochemistry 2007 296(1-2) 77-84
60 Michael C Moulton Laura K Braydich-Stolle Mallikarjuna N Nadagouda Samantha
Kunzelman Saber M Hussain Rajender S Varma Nanoscale 2010 2 763-770
61 Goya DV Matijevic E Colloids and Surfaces A 1999 146 139
62 Velikov KP Zegers GE van Blaanderen A Langmuir 2003 19 1384
63 Goldenberg L M Wagner J Stumpe J Paulke B-R Goumlrnitz E Langmuir 2002 18
5627-5629
59
64
Banerjee S Gopal J Muraleedharan P Tyagi A K Raj B Curr Sci 2006
901378ndash1383
65 Bogomolov V N Kudinov E K Firsov Y A Sov Phys Solid State 1968 35 555
66 Kudo A Miseki Y Chem Soc Rev 2009 38 253ndash278
67 Gaj T Meyer SC Ghosh I Protein expression and Purification 2007 56 54-61