engineering polymer molecules: twirling dna rings and loop polymers rochish thaokar iit bombay...
TRANSCRIPT
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Engineering polymer molecules: Twirling Engineering polymer molecules: Twirling DNA Rings and loop polymersDNA Rings and loop polymers
Rochish ThaokarIIT Bombay
Collaborators:Igor Kulic, University of PennsylvaniaHelmut Schiessel, Univ Leiden, The Netherlands
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Nano-sized gadgets doing mechanical work
Nano gears, lever arms, wheels=> nanomachine
Can we make Nanomotors
NanomachinesNanomachines
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MedicineMedicine
Cancer recognising nanovehicles
“repair” cells, bones,tissues and reinforcement
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Kinesin motor proteins moving on
Microtubules
Are there biological nanomachinesAre there biological nanomachinesBiological molecular motors!!
Myosin and actin are responsible for
muscle contraction
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What are the properties of the material What are the properties of the material making a nanomachinemaking a nanomachine
StabilitySelf assembly abilityModularity and ReplicabilitySwitchabilityExperimentally tractable
DNA
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The DNA nanomachines available today!!The DNA nanomachines available today!!
DNA Hybridisation
Conformationalchanges
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Four orders of magnitude slower than their biological counterparts
Large switching times: 103 s
Drawbacks of the current nanomachinesDrawbacks of the current nanomachines
Structural complexityCan we come up with a simpler nanomachineWith Sub-second switching timesSwimming as fast as a bacteria (100 µ/s)
A DNA MINIMPLASMID
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Has three degrees of freedom
is the angle of rotation around its centerline
We are interested in the degree of freedom
In thermal equilibrium, the ring fluctuates in an unbiased manner
There is no directed motion
A DNA MINIMPLASMIDA DNA MINIMPLASMID
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U(x)
Diffusion
x
x
U(x)
No Net Motion
x
U(x)
Basic Brownian Ratchet (Potential Basic Brownian Ratchet (Potential ratchet)ratchet)
No Net current for a symmetric potential
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U(x)
Diffusion
x
x
U(x)
Net Motion
x
U(x)
Basic Brownian Ratchet (Potential Basic Brownian Ratchet (Potential ratchet)ratchet)
Energy input from the switching potential U(x) used to rectify random thermal motion
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U(x)
Diffusionx
x
U(x)
Net Motion
x
U(x)
Basic Brownian Ratchet (Thermal ratchet)Basic Brownian Ratchet (Thermal ratchet)
Energy input from the switching Temperature T(t) used to rectify random thermal motion
T=Finite
T=0
T=0
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Nature uses and designs the ratchet to extract useful work from Thermal fluctuations
Some biological molecular motors described by Brownian ratchets
The Kinesin-Microtubulemotion is ratchet motion: ATP provides the energy, +/-ends of microtubule ,conformation change, theasymmetry
Examples in NatureExamples in Nature
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Can we make use of the ratchet principle Can we make use of the ratchet principle to move our DNA minplasmid ?to move our DNA minplasmid ?
The DNA is a complicated molecule:
Neucleotides, Deoxiribose sugar and Phosphate
Double Helix, Highly charged polymer
Coarse grain the DNA: Its a Semiflexible polymer
<t(s) t(s+l)> ~ 0 Flexible ~ Semiflexiblee l lp
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What is the most general form of the What is the most general form of the hamiltonian??hamiltonian??
Consider a circular ring: = /2; =s/R
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Consider a Thermal Ratchet:
T(t)=To (1+A Sin f t)
Current:
The Hamiltonian is asymmetric in variable
is a fluctuating variable and so governed by Fokker Planck equation
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l1=l2 =45, 50 nm;
200 nm;
R/r=10;
R=10 nm
f= 1000 Hz
= 200 rad/s
The ring rotates around its centerlineThe ring rotates around its centerline
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How can we heat up the DNA so fast?How can we heat up the DNA so fast?
Ultrasound
Metal Nanocrystals covalently attached to DNA
Can the twirling ring translate?Can the twirling ring translate?
Fluid Mechanics !! Typical Reynolds numbers: 10^(-3)
Low Reynolds number hydrodynamics!!
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All the fundamental solutions satisfy stokes equation
The torus should be force free and torque free
Construct solution consisting rotlets:
Stokes Fundamental solutionStokes Fundamental solution
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How fast does the ratchet moveHow fast does the ratchet move??50 nm/s
Potential ratchet: E=Eo(1+A sin f t)
A can be as high as 0.3
Can be realised by operating the system close to DNA duplex melting
temperature
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The ring moves at around 5 microns/second!!The ring moves at around 5 microns/second!!
As good as the speed of an amoebaAs good as the speed of an amoeba
Generates Torques (kbT) and forces (fN)Generates Torques (kbT) and forces (fN)
note: note: Rotational diffusion can alter the courseRotational diffusion can alter the course
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Life at Low Reynolds NumberLife at Low Reynolds Number
Inertial negligible, Quasi-static ,reversible equations ref : Life at Low Reynolds number : Purcell
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Comparison of Torus translational velocity
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DNA on rails
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Interaction between two torri
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Can there be flow induced organisation
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ConclusionsConclusions
A DNA Miniplasmid can be a NanomachineA DNA Miniplasmid can be a Nanomachine
Intrinsic curvature and anisotropy for asymmetry in potentialIntrinsic curvature and anisotropy for asymmetry in potential
A Thermal ratchet can cause it move at around 50 nm/sA Thermal ratchet can cause it move at around 50 nm/s
A potential ratchet can make it move at 10 micros/sA potential ratchet can make it move at 10 micros/s
Switching times is Smoluchowski times and so very fastSwitching times is Smoluchowski times and so very fast
We can possibly explain Purcell's swimming animalWe can possibly explain Purcell's swimming animal
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References
1.1. Igor M Kulic, Igor M Kulic, RochishThaokarRochishThaokar, Helmut Schiessel, , Helmut Schiessel, “Twirling DNA “Twirling DNA rings- Swimming Nanomotors ready for kick start”,rings- Swimming Nanomotors ready for kick start”, Europhysics Letters, Europhysics Letters, 72,527-533, 200572,527-533, 2005
2.2. I.M.Kulic, I.M.Kulic, Rochish ThaokarRochish Thaokar, Helmut Schiessel, , Helmut Schiessel, “A DNA ring acting as a thermal ratchet”, J Phys Cond Matt, 17, S3965, 2005 J Phys Cond Matt, 17, S3965, 2005
3.3. Rochish ThaokarRochish Thaokar, Igor Kulic, Helmut Schiessel, , Igor Kulic, Helmut Schiessel, ““Hydrodynamics of a rotating torus”, submitted to Physics of Fluids submitted to Physics of Fluids
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Force extension study of Loop Force extension study of Loop DNADNA
Collaborators:
Herve Mohrbach, Univ Leiden, The Netherlands
Vladimir Lobaskin, MPIP-Mainz Germany
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Help study the structure and conformation of individual molecules
Where do these loop polymers occur:Where do these loop polymers occur:
a) Freely sliding linker proteins stabilizes a DNA loop
b) A rigid ligand with opening angle alpha causes a kink in DNA
c) Tangentially anchored DNA stretched by an AFM tip
Why Study force-extension curveWhy Study force-extension curve
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Manipulations by a magnetic trapManipulations by a magnetic trap
Small magnets allow for stretching and twisting a DNA molecule. By measuring the distance of the bead to the surface and its fluctuations x2, one deduces the DNA’s extension, l and the stretching force, F.
magnets
magnetic bead
DNA
surfaceF =
k BT
2 l
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Theory of Force-extension curves Theory of Force-extension curves
Straight chainsStraight chains
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T=0 state has Enthalpy Ho
Thermal Fluctuations lead to entropic contributions
H=Ho+H Q=Qo*Q1
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Q1 is entropic part of partition functionQ1 is entropic part of partition function
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How to calculate the partition function How to calculate the partition function for fluctuationsfor fluctuations
Polymer problems can be suitably mapped to quantum mechanical problems
A vast literature exists for QM problems
An analogy and variable transformation can directly give the Partition function
Quantum Mechanics
Polymer Physics
Variable
transformatio
n
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Calculation of Q1Calculation of Q1
Exponential Partition function contributes to Force extension
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Wormlike chain model: lp is the persistence length
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Used to Fit DNA, Proteins etc.
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Looped chainsLooped chains
sqrtkbT lp/F) The enthalpic part is non-trivial
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Inplane-out of plane fluctuations contribution Inplane-out of plane fluctuations contribution
to entropic part to entropic part Is there a quantum mechanical analogueIs there a quantum mechanical analogue
The eigen values allow us to evaluate the partition functionThe eigen values allow us to evaluate the partition function
There is discrete and continuous spectrum of eigen valuesThere is discrete and continuous spectrum of eigen values
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Q=Q(Enthalpic,loop)*Q(Entropic,loop)
Q(Entropic,kink) =Q(Entropic,straight)*Q1
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Q=QQ=Q(Enthalpic,loop(Enthalpic,loop)*Q)*Q(Entropic,loop)(Entropic,loop)
QQ(Entropic,kink(Entropic,kink)) =Q =Q(Entropic,straight)(Entropic,straight) *Q1 *Q1
Q=QQ=Q(Enthalpic, loop(Enthalpic, loop))*Q*Q(Entropic,straight)(Entropic,straight) *Q1 *Q1
Results:Results:
Q1Q1==sqrtsqrt((4 lp L/4 lp L/^2^2) ) Q1 is linearQ1 is linear
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Partition function for the unstable loop can be Partition function for the unstable loop can be
resolvedresolved
The entropic contribution are logrithmicThe entropic contribution are logrithmic
(courtsey Herve Mohrbach)(courtsey Herve Mohrbach)
The force extension can be given by a WLCThe force extension can be given by a WLC
The apparent persistence length: l*=lp (1+8 lp/L)^(-2)The apparent persistence length: l*=lp (1+8 lp/L)^(-2)
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The entropic contribution of kinks and loops is logrithmic in the high stretch limit
Enthlapic contribution is important and is easily calculated
The force extension curves for DNA with adsorbed proteins and the AFM tip
uncertainty can be addressed
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Simulation vs theorySimulation vs theory
(courtsey Vladimir Lobaskin)(courtsey Vladimir Lobaskin)
Force-extension curvesForce-extension curves
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ConclusionsConclusions
A semiflexible chain which is looped or non-straight can be A semiflexible chain which is looped or non-straight can be
expressed by a WLC modelexpressed by a WLC model
The persistence length is re-normalizedThe persistence length is re-normalized
The renormalisation is due to enthalpic effectsThe renormalisation is due to enthalpic effects
The theory explains discrepancies in the force-extension The theory explains discrepancies in the force-extension
curves semiflexible polymers, looped and kinked DNAs and curves semiflexible polymers, looped and kinked DNAs and
DNA protein complexesDNA protein complexes
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Future WorkFuture Work
A Lattice Boltzmann-Brownian dynamics method to compute the flow fields for non-slender torus
Analytical and simulation model for interaction of two torri
Interaction of an ensemble of torri
Effect of thermal fluctuations on the single torus
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References
Igor Kulic, H Mohrbach, V Lobaskin, Rochish Thaokar, Helmut Igor Kulic, H Mohrbach, V Lobaskin, Rochish Thaokar, Helmut Schiessel, Schiessel, “Apparent persistence length renormalisation of a Bent DNA”, Physical Review E, 72, 041905-1-5,2005 Physical Review E, 72, 041905-1-5,2005
Igor Kulic, H Mohrbach, Rochish Thaokar, Helmut Schiessel, Igor Kulic, H Mohrbach, Rochish Thaokar, Helmut Schiessel, “Equation of state of a looped DNA”,“Equation of state of a looped DNA”, Physical Review E (Under Physical Review E (Under Review)Review)