2. sans basics - nist · 6/12/2012 10 0 20 40 60 80 100 120 140 0 0.05 0.1 0.15 0.2 0.25 0.3...
TRANSCRIPT
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SANS BASICS
Boualem Hammouda
National Institute of Standards and Technology Center for Neutron Research
OUTLINE• 1. The SANS Technique
• 2. SANS Data AnalysisStandard Plots (Guinier, Porod)SANS ModelsInverse Fourier TransformShape Reconstruction Method
• 3. SANS Research TopicsA- Phase Transitions in Pluronic P85 SolutionsB- Role of Chirality in Peptide BiogelsC- Structure of SDS Micelles
• 4. Final PointsVSANS and USANSFinal Words
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1 – The SANS Technique
The NIST Center For Neutron Research
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Incident Beam
Area Detector
Scattered BeamSample Q
SourceAperture
SampleAperture
MonochromaticNeutron Beam
Monochromation Collimation Scattering Detection
2
sin4
Qneutron
wavelength
scattering angle
Small-Angle Neutron Scattering
Nanoscale Structures
0.010.001 0.1 1
Scattering Variable Q (Å-1)
Length Scale (Å)
1001000 10
10-410-5
104105106
Polymers
ComplexFluids
Biology
SANSUSANS
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d
d
d
)Q(d)Q(I incohcoh
COHERENT INCOHERENT
- Q-independent- no info. about structure
~ Contrast factor = (A‐B)2- Info. about structure
Scattering length density:volume
length scattering
v
b
A
AA
SANS Cross Sections
Zero contrast
Multiple contrasts Contrast match
Finite contrast
The Contrast Match Method
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2 –SANS Data Analysis
• Standard Plots (Guinier Plot, Porod Plot)
• SANS Models
• Inverse Fourier Transform
• Shape Reconstruction Method
SANS Data Analysis
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0.0001
0.001
0.01
0.1
1
10
0.001 0.01 0.1 1
Cylinder with Rg2
= 100 Å and Rg1
= 10 Å
Fo
rm F
act
or
P(Q
)
Scattering Variable Q (Å-1)
1/Q1
1/Q4
1/Q0 Low-Q Guinier Region
Intermediate-Q Guinier Region
Porod Region
Guinier-Porod Regions Guinier Plots
2
R
12
LRg
yields slope22
22
-1
-0.8
-0.6
-0.4
-0.2
0
0 0.0001 0.0002 0.0003 0.0004
Ln
[P(Q
)]
Q2
2
RRg
yields slope2
21
-7
-6.5
-6
-5.5
-5
-4.5
0 0.01 0.02 0.03 0.04
Ln
[Q*P
(Q)]
Q2
SANS Models
cross section
volume fraction
contrastfactor
Macromolecules Particles
Structure FactorSI(Q)
Form FactorP(Q)
Structure FactorSI(Q)
Form FactorP(Q)
form factor
structure factor
Random Phase Approximation Ornstein Zernike
particle volume
)Q(S )Q(PVd
)Q(dIA
2BAA
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U(r)
r
Hard Sphere
Screened Coulomb
Square Well
Particle Structure Factor –The Ornstein-Zernike Equation
)Q(S )Q(PVd
)Q(dIA
2BAA
Form FactorP(Q)
StructureFactorSI(Q)
10-5
0.0001
0.001
0.01
0.1
1
10
0.1 1 10
Percus-Yevick Model for Sphere
Form Factor P(Q) Struct. Fact. S
I(Q)
P(Q)*SI(Q)
Fo
rm F
acto
r an
d S
tru
ctu
re F
acto
r
QR
Fourier Transform
)r(PQr
)Qrsin(r4dr
V
1)r(P ]r.Qiexp[rd)Q(P 2
0P
3
3
R
r
16
1
R
r
4
31)r(P
r
r’
R
Fourier transform:
Radial pair correlation function:
Density-density correlation function:
)]r'r.(Qiexp[n
)'r(n)r(n'rdrd
n
)Q(n)Q(n)Q(P
22
0
0.2
0.4
0.6
0.8
1
0 0.5 1 1.5 2
Sphere
P(r)
(r/R)2*P(r)
Pai
r C
orr
ela
tio
n F
un
ctio
n
r/R
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A- Phase Transitions in Pluronic P85 Solutions
B- Role of Chirality in Peptide Biogels
C- Structure of SDS Micelles
3. SANS Research Topics
A - Phase Transitions in Pluronic P85 Solutions
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Dissolved Unimer(low temperature)
Formed Micelle(high temperature)
PEO
PEO
PPO
hydrophobic
hydrophilic
PEO PPO
PEO
P85: EO26PO40EO26
Pluronics
EO:-CH2CH2-O-
PO:-CH(CH3)CH2-O-
0.1
1
10
100
0.01 0.1
0.5 % P85 in d-Water
100 oC
90 oC
70 oC
50 oC
10 oC
Sca
tter
ing
Inte
nsi
ty (
cm-1
)
Scattering Variable Q (Å-1)
1/Q4
1/Q1
1/Q2
1/Q0
unimers
sphericalmicelles
cylindricalmicelles
lamellarmicelles
1/Q5/3
Pluronic Micelles
lamellarmicelles
cylindricalmicelles
sphericalmicelles
unimers
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0
20
40
60
80
100
120
140
0 0.05 0.1 0.15 0.2 0.25 0.3
P85/d-Water
demixed lamellae formation linecylindrical-to-lamellar micellesspherical-to-cylindrical micellesunimers-to-spherical micelles
Tem
per
atu
re (
oC
) P85 Fraction
unimers
spherical micelles
cylindrical micelles
lamellar micelles demixed lamellae
paracrystallinespherical micelles
paracrystallinecylindrical micelles
Phase Diagram
0.1
1
10
100
1000
20 30 40 50 60 70 80 90 100
0.5 % P85/d-Water
Gu
inie
r F
acto
r
Temperature (oC)
26 oC 62 oC 82 oC
sphericalmicelles
cylindricalmicelles
lamellarmicelles
Core-Shell Spherical Particles Model
core region A
shell region Bsolvent region C
10% P85 Pluronic/D2O, 40 oC
RA=43.9 Å
RB=72.0 Å
C = 6.4*10-6 Å-2
B = 5.9*10-6 Å-2
A = 1.7*10-6 Å-2
Fits yield
)Q(SQR
)QR(j3V
QR
)QR(j3V
V
N
d
)Q(dI
2
B
B1BACB
A
A1ABA
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Core-Shell Spherical Particles
3A
AODEOPOagA
R3
4
]y.f.b52f.b.52b40[N2
)RR3
4
]y).f1.(b.52)f1.(b.52[N
3A
3B
BODEOagB
2
AODEOPOag3
A y.v.f.52v.f.52v.40.NR3
42
BODEOag3
AB y.v).f1.(52v).f1.(52.N)RR(3
42
In the core:2,795 PPO monomers690 PEO monomers490 D2O molecules
In the shell:2,943 PEO monomers34,167 D2O molecules
Material Balance Equations: Results for 10% P85 at 40 oC:
B- Role of Chirality in Peptide Biogels
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Faraday Rotation
Substances rotate linearly polarized light to the left (L-type) or to the right (D-type)
- A molecule is chiral if it is different from its mirror image
- Human hands are chiral
- Non-biological substances are heterochiral . They can be of the L-type or D-type
- Biological substances are homochiral. They are either of the L-type or of the D-type
- Proteins are of the L-type. Sugars are of the D-type. DNA is of the D-type. The reason is still a mystery
Chirality
Right handedLeft handed
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- Proteins are responsible for most biological function. They are made out of peptides. Peptides are made out of amino acids. There are 20 amino acids.
- Examples of amino acids include Lysine (K), Glutamate (E), Tryptophan (W) and Alanine (A)
- Most proteins rotate polarized light to the left. They are left handed or L-type
Proteins
DNA- DNA is the blueprint for life. It is the template for the synthesis of proteins
- DNA is made out of nucleotides. There are 4 DNA nucleotides: A, C, T and G
- The human genone contains 6 billion nucleotides making up some 23,000 genes
- Most DNA rotate polarized light to the right. They are right handed or D-type
- Peptides can be synthesized to be L-type or D-type
- Series of L-type and D-type short peptide sequences (11 amino acids) were synthesized.
- These were combined to give L-D- or D-L- heterochiral mixtures and L-L- or D-D- homochiral mixtures
- The resulting gels were investigated using mechanical testing (shear response) and SANS measurements
Peptide Biogels
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Mechanical Testing
- Heterochiral samples gel faster. Homochiral samples are slow to gel.
- Homochiral gels are initially weaker then become stronger
0 10 20 30 40 50100
101
102
103
104
105
Ela
stic
Modulu
s, P
a
Time, hrs
heterochiral
homochiral
SANS Data
Homochiral
Heterochiral
- Heterochiral gels scatter differently from homochiral ones
- They are all characterized by fibrilar structure
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SANS Data Analysis
Homochiral
Heterochiral
Heterochiral
Homochiral
- Homochiral fibers are thicker and denser than heterochiral ones
Shape ReconstructionFiber cross sections
Inverse FourierTransform
heterochiralhomochiral
webFiber
- Peptide biogel is formed of fibers joined by a web
Fiber-Web Structure
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- Chirality plays a role in the mechanical properties and structure of biogels
- Homochirality confers higher strength (shear modulus) and yield stress value. Right-right hand-shake is stronger.
- Heterochirality confers faster gelation kinetics
- Biogel structure consists of main fibers held together by a web of cross fibers
- Fibers for homochiral biogels are thicker and denser
- Advantages conferred to homochirality lead to enhanced stability
Results
C- Structure of SDS Micelles
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- Surfactants are formed of a hydrophilic head and a hydrophobic tail
- Micelles form when enough surfactants aggregate (above the critical micelle concentration or CMC)
- SDS surfactants form micelles in water (or deuterated water)
Micelle Formation
0.1
1
10
0.01 0.1
68 oC
20% SDS10% SDS5% SDS2% SDS1% SDS0.5% SDS
Sca
tte
red
In
ten
sit
y (
cm-1
)
Scattering Variable Q (Å-1)
SANS from SDS Micelles
- Ellipsoidal micelles form
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0.1
1
10
0.01 0.1
5 % SDS, 49 oC
Model FitSANS Data
Sca
tte
red
In
ten
sit
y (
cm-1
)
Scattering Variable Q (Å-1)
Bd
)Q(d
Q
A)Q(I
ellipsoidsn
)Q(S)Q(PV2
ellipsoidsd
)Q(dIP
Ellipsoid Micelles Model Fit
- Power law (low-Q) + ellipsoidal micelles (high-Q) model fits well
1.5 104
2 104
2.5 104
3 104
3.5 104
4 104
4.5 104
280 300 320 340 360
10 % SDS5 % SDS 2 % SDS 1 % SDS 0.5 % SDS
Elli
ps
oid
Vo
lum
e (Å
3 )
Temperature (K)
Some Fit Results
- Micelles become smaller at higher temperatures and lower volume fraction
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10
15
20
25
30
35
-0.1 0 0.1 0.2 0.3 0.4 0.5 0.6
1% SDS/d-Water, 21 oC
Ra Rb
Elli
pso
id H
alf
Ax
es (
Å)
NaCl Salt Fraction (mol/L)
More Fit Results
- Salt addition affects lateral growth only
-0.2
0
0.2
0.4
0.6
0.8
1
0 20 40 60 80 100
1 % SDS/d-Water
SDS fraction in the micellesD
2O fraction in the micelles
SD
S a
nd
D2O
Fra
cti
on
s in
th
e M
icel
les
Temperature (oC)
Material Balance Equations
- SDS surfactant fraction remains constant above the CMC
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SDS MASS FRACTION (%)
T E M P E R A T U R E
(oC)
25
50
75
100
25 50 75 10000
lamellar phase
intermediates
spherical micelles
hydrated SDS crystals
hexagonalphase
intermediates+ crystals
hexagonal phase+ crystals
lamellar phase+crystals
Phase Diagram
- SDS/water phase diagram from calorimetry
4. Final Points
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Upgrade and VSANS
30 m SANS
Present Guide Hall
New Guide Hall
30 m SANS
40 m VSANS
10 m SANS
USANS
ConfinementBuilding
USANS Instrument
SANS, VSANS and USANS Ranges
VSANS
0.01
1
100
104
106
108
1010
10-5 0.0001 0.001 0.01 0.1 1
4% PEO/d-Ethanol,
Mw=42,900 g/mole, T=25oC
USANS DataSANS Data
Sca
tte
red
In
ten
sity
(cm
-1)
Q (Å-1)
SANS
USANS
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0.0001
0.01
1
100
104
106
108
1010
10-5 0.0001 0.001 0.01 0.1 1
Crosslinked CTVB Micelles
gel with no excess oil gel with excess octane gel with excess toluene
Sca
tte
red
In
ten
sity
(c
m-1
)
Q (Å-1)
SANS and USANS Data
VB-
CTA+
Final Words
THE SANS PROGRAM AT NIST
200 experiments per year
15 theses per year
80 publications per year
REFERENCES- B. Hammouda, “Probing Nanoscale Structures – The SANS Toolbox”, (2009). Book available online.- M. Taraban, Y. Feng, B. Hammouda, L. Hyland and B. Yu, “Chirality-Mediated Mechanical and Structural Properties ofOligopeptide Hydrogels”, Chemistry of Materials (2012)
ACKNOWLEDGMENTSSteve Kline, Marc Taraban, Bruce Yu
http://www.ncnr.nist.gov/staff/hammouda/