Lecture Script Polymer Sci II Colloid Stability
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Transcript of Lecture Script Polymer Sci II Colloid Stability
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A state of subdivision in
which the particles,
droplets, or bubbles
dispersed in another
phase have at least one
dimension between 1 and
1000 nm
all combinations are
possible between :
gas, liquid, and solid
W. Ostwald
Colloidal systems
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Surface area of colloidal systems
Cube (1cm; 1cm; 1cm)after size reduction to an edge length of 500 nm:
surface area of 60 m2
Spinning dope (1 cm3)
after spinning to a fibre with diameter of 1000 nm:
fiber length of 1273 km
1 liter of a 0.1 M surfactant solution:
interfacial area of 40000 m2
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Surface atoms [in %]
in dependence on the particle size [in nm]
0
10
2030
40
50
60
7080
90
100
20 10 5 2 1
part of surface
atoms in %%
nm
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Colloidal systems
have large surface areas
surface atoms become dominant
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Colloid stability
Colloidal gold: stabilized against coagulation !
Creme: stabilized against coagulation !
Milk: stabilized against coagulation !
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ParticleParticle interactions
Interaction Energy ( Vtot)Distance of
Separation (d) Relationship
d
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DLVO - Theory
1940 Derjaguin; Landau; Verwey; Overbeek
Long range attractive van der Waals forces
Long range repulsive electrostatic forces
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DLVO Theory
Van der Waals attractive energy
a) between two plates:
b) between two spheres:
2
.
12 d
AVattr WaalsderVan
d
aAV
attr
WaalsderVan12
.
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Double layer models
Helmholtz
Gouy Chapman
Stern
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Gouy Chapman model
planar double layer
Ions as point charges
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Electrolyte theory
kT
xez
iii
i
enezxd
xd
0
2
24
I distribution of ions in the diffuse double layer
(Boltzmann equation)
II equation for the room charge density
III Poisson relation
Aus I, II und III folgt:
Poisson
Boltzmann - relation
kT
xezenxn iii
xnezx iii
0
2
24 x
xd
xd
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Solution of the P-B equation
xekx
xxd
xd
k
k
0
2
2
2
For small potentials (< 25 mV) :
Integrable form
kT
xez
i
ii
i
enezdx
xd
0
2
24
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DLVO Theory
Electrostatic repulsive energy
Resulting repulsive overlap energy
a) Between two plates:
c volume concentration of the
z valent electrolyte
b) Between two spheres
drep
elektrost ekTc
V k
k
64
.
2
2
2
22
0
22
.
1
18
kT
ze
kT
ze
drep
elektrost
e
ee
ze
TkV
k
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Vtot(d)= Vattr(d) + Vrep(d)
Vvan der Waals
= - A a / 12 d Velectrost.
= k e-kd
AHamaker constant
aparticle radius
d
distance between the particles
1/k - thickness of the double-layer
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Electrostatic stabilization
stabilized against coagulation
Kinetically stable state
energetic metastable state in the
secondary minimum
with an energy barrier
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Critical coagulation concentration (CCC)
The energy barrier disappears by adding a
critical amount of low molecular salts
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DLVO Theory
(CCC)
Vtot / dd = 0 Vtot = 0
for two spheres:
2
266
3
0
3553
2
2
2
2
122
0
22
1
1
4
1039,3
121
18
kT
ze
kT
ze
kT
ze
kT
ze
e
e
Aze
Tkccc
daA
e
eeze
Tk
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DLVOTheory
(CCC)
For two spheres the ccc should be related to
the valency (1 : 2 : 3) of the counterions as:
1000 : 16 : 1,3
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CCC of a colloidal dispersion as a function of
the salt concentration
AlCl3
CaCl2
MgCl2
KCl
NaCl
electrolyte
1,79,3 10-5
136,5 10-4
137,2 10-4
10005,0 10-2
10005,1 10-2
Schulze-Hardy-ratioCCC of a
Arsensulfid -Dispersion
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Steric stabilization
What will be happen when we add polymers
to a colloidal dispersion ?
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ParticleParticle interactions
Polymer adsorption layer
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ParticleParticle interactions
Overlap of the
polymer adsorption layer
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Overlap of the adsorption layer
Osmotic repulsion
Entropic repulsion
Enthalpic repulsion
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Sterically stabilized systems can
be controlled by
The thickness of the adsorption layer
The density of the adsorption layer
The temperature
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Stabilization and destabilization in
dependence on the molecular
weight of the added polymer
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Stabilization and destabilization in
dependence on the
polymer-concentration