kyongok kang (fz-juelich) a (short) introduction to colloids electric-field induced phase...
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![Page 1: Kyongok Kang (FZ-Juelich) A (short) introduction to colloids Electric-field induced phase transitions, dynamical states and non-equilibrium critical behaviour](https://reader036.vdocuments.us/reader036/viewer/2022062423/56649eef5503460f94bff3fa/html5/thumbnails/1.jpg)
Kyongok Kang (FZ-Juelich)
A (short) introduction to colloids
Electric-field induced phase transitions, dynamical states and non-equilibrium critical behaviour in concentrated suspensions of rods
From David pine’s webpage
Jan Dhont ICS-3
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Introduction to Colloids
Colloidal particles are “aggregates” with linear dimensions in the size range of 1 nanometer – 20 microns
What are Colloids ?
colloids are much larger than fluid molecules
colloids exhibit vivid thermal motion
sphere diameter 500 nm“hydodynamic interactions”
“Brownian motion”
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Introduction to Colloids
Colloidal particles are “aggregates” with linear dimensions in the size range of 1 nanometer – 20 microns
What are Colloids ?
colloids exhibit vivid thermal motion
sphere diameter 500 nm
colloid
water molecules
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Introduction to Colloids
Colloidal particles are “aggregates” with linear dimensions in the size range of 1 nanometer – 20 microns
What are Colloids ?
colloids exhibit vivid thermal motion
sphere diameter 500 nm
colloid
water molecules
Same laws of Thermodynamics and Statistical Physics
Phase transitions
You don’t have to learn anything new to understand colloids (in principle)
Brownian motion is nothing but thermal motion
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r
V(r)
---- - - --
----
- - - ----
----
Direct interactions can be tuned “at will”
Crystallization (FCC)Glasses
Liquid-gas coexistenceAggregationGels
Crystallization (FCC and BCC)Electric fields
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Crystallization of “hard spheres”
P.N. Pusey, E. Zaccarelli, C. Valeriani, E. Sanz, W.C.K. Poon, M.E. Cates, Phil.Transactions A, 367, 4993 (2009); arXiv:0908.1663v1 [cond-mat. Mtrl-sci]
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fluid
gel
H. Verduin, J.K.G. Dhont, J. Coll. Int. Sci. 172, 425 (1995)
“sticky spheres”
(taken from Eric Weeks webpage)
binodal
spinodal
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M.E. Leunissen et al., Nature 437, 235 (2005)
Mixture of charged and uncharged colloids
NaCl-type crystal
NiAs-type crystal
---- - - --
----
- - -----
----
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Other shapes : rod-like colloids
fd virus : L = 880 nm D = 7 nm P = 3000 nm
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Sphere diameter 100 nmRod length 900 nm
Adams et al., Nature,1998
Mixtures of rods and spheres
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F.M. van der Kooij, M. Vogel, H.N.W. Lekkerkerker, Phys. Rev. E 62, 5397 (2000)
disks patchy colloids
From David pine’s webpage
star-like polymers(like DNA-colloids)
from David Pine’s webpage
transient, non-equilibrium forces
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-COOH
-COOH
-COOH
-COOH
-COOH-CO
OH
-COOH
-CO
OH
-CO
OH
-CO
OH
-CO
OH
-COOH
-COOH
-COOH-COOH -COOH -C
OO
H
-CO
OH
-CO
O-
-CO
O-
-COO-
-COO-
-COO-
-COO-
-COO-
-COO--CO
O-
-COO-
-CO
O-
-CO
O-
-COO-
-COO-
-COO- -COO- -CO
O-
-CO
O-
H+
H+
H+
H+
H+
H+
H+
Electric double layer / layer of condensed ions :
no dissociation : low S low U
dissociation : high S high U
minimization of F=U -TS
-COOH
-COO-
-COOH
-COOH
-COO--CO
OH
-COO-
-CO
OH
-CO
O-
-CO
OH
-CO
OH
-COO-
-COOH
-COO--COOH -COO- -C
OO
H
-CO
O-
H+
H+
H+
H+
H+
H+H+H+
1 nm-10 micron
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Debye lengthscreening length
Electric double layer
ionconcentratsalt/1~1
r
r}exp{~
charge density
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diffuse electric double layer
thin layer of “condensed” ions
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At sufficiently low frequencies (< 10 kHz) : - double layers are polarized - the layer of condensed ions is polarized - field-induced association-dissociation of condensed ions - electro-osmotic flow is induced
--
- --
-
-
---
-
-
-
+ +
+
+
++
++++
+
+-
-
-
-- - -
-
-
-
---
+
+
++++
++
+
+
++
Field-induced colloid-colloid interactions : - electrostatics - hydrodynamics
E
Electric-field induced phases, dynamical states , and critical behaviour in suspensions of rod-like charged colloid
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fd virus : L = 880 nm D = 7 nm P = 3000 nm
- 0.16 mM TRIS/HCl buffer (Debye length is 27 nm) - fd concentration is 2.0 mg/ml = within the isotropic-nematic two-phase region- At high ionic strength, the nematic phase is a cholesteric
100 101 102 1030
2
4
6
E[V/mm]
[Hz]
*N
N
HD
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polarizer
analyzer
10 x
G
sample
function generator lightsource
DIC
CCD
L = 1.5 mm
K. Kang, J.K.G. Dhont, Soft Matter 6, 273 (2010)
Concentration : 2.0 mg/ml two-phase, isotropic-nematic coexistence = 26 c*
isotropic
nematic
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100 101 102 1030
2
4
6
E[V/mm]
[Hz]
*N
N
HD
Nematic + Isotropic
200 micron
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100 101 102 1030
2
4
6
E[V/mm]
[Hz]
*N
N
HD
Nematic + Chiral-nematic
200 micron
a chiral nematic is also found at high ionic strengthsand at higher f-concentration without an electric field
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100 101 102 1030
2
4
6
E[V/mm]
[Hz]
*N
N
HD
200 micron
Uniform homeotropic alignment
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100 101 102 1030
2
4
6
E[V/mm]
[Hz]
*N
N
HD
200 micron
Uniform homeotropic alignment
order parameter (S=0.48) and diffusion coefficients are independent of field strength and frequency
no charge-polarization
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100 101 102 1030
2
4
6
E[V/mm]
[Hz]
*N
N
HD
200 micron
Melting and forming of nematic domains
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E0
dissociation of condensed ions
increase of ionic strength
aligned state is unstable
decay towards the isotropic state
association of condensed ions
decrease of ionic strength
de-aligned state is meta-stable or unstable
orientational order increases
rotation of the director towards the external field
(i)
(ii)(iii)
(iv) (v)
Origin of the dynamical state:
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100 101 102 1030
2
4
6
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100 101 102 1030
2
4
6
E[V/mm]
[Hz]
*N
N
HD
Critical behaviour: - Domain size diverges - Characteristic time for melting/forming diverges
200 micron
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I
t
0 10 20 300.0
0.2
0.4
0.6
0.8
1.0
CV
time [s]
3.26 V/mm
3.78
4.09
5.77
( ) expV
tC t
2
( ( ) ( ) ) ( (0) (0) )( )
( (0) (0) )V
I t I t I IC t
I I
100 101 102 1030
2
4
6
characteristic time for melting/forming
“video-image correlation function”:
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d : power-law : power-law
d : logarithmic
: power-law
: logarithmic
d : finite
E
1.39E 0.18 1.29E
d 0.15
0.65 0.15
N*
DH
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kHzL
kHzD
L
H
D
10001
11
2
2
L
Polarization for parallel orientation only important when :
Hydrodynamic interactions are instantaneous when :
1/
1
Ld
LLong rods :
time to diffuse over the length of the rod
frequency of the external field
diffusion coefficient of salt ions
time for a shear wave to propagate of a distance L
specific mass
shear viscosity
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100 101 102 1030
2
4
6
E[V/mm]
[Hz]
*N
N
HD
polarization (neglect hydrodynamic interactions)
hydrodynamic interactions (neglect polarization)
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Theory low frequencies - polarization of a single particle (cooperation with Jerry Manning)
- calculation of the pair-interaction forces- include these forces in the Smoluchowski equation (no HI: )- account for the field-induced association-dissociation of condensed ions
high frequencies (cooperation with Bogdan Cichocki)- flow induced by a single, unperturbed equilibrium double layer- “active” hydrodynamic interaction functions- analyze the Smoluchowski equation + “active” hydrodynamic + unperturbed direct interactions
ˆˆˆ PP
PPHP
t ,
pdf for positions and orientations
hydrodynamic interactions
direct interactions
rotation operator
gradient operator
Smoluchowski equation: (or : “the overdamped Liouville equation”)
rD
uuIDH
0
0ˆˆˆ,
0 E
diffusion-migration on a surface
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movies are 10 times accelerated200 um
N*-formation kinetics after a frequency quench from the H-phase
100 101 102 1030
2
4
6
E[V/mm]
[Hz]
*N
N
HD
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Thank you for your attention
200 um movies are 10 times accelerated