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Colloidal Aggregation FDSC400

Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

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Page 1: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Colloidal Aggregation

FDSC400

Page 2: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Goals

• Aggregation rate

• Interaction potentials

• Electrostatic repulsion

• Van der Waals attraction

• DVLO theory

• Steric repulsion

Page 3: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Aggregation Rate

• Second order reaction (fast kinetics):

or

2P P2

2][Pkdt

dP

Page 4: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Smoulokowski Kinetics

• Gives the rate of collision of freely diffusing particles

• We know the diffusion coefficient of spheres

• Combining

Drk 8

r

kTD

6

34kT

k

D =

dif

fusi

on c

oeff

icie

nt, r

= r

adiu

s,

=

cont

inuo

us p

hase

vis

cosi

ty

Page 5: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Slow Kinetics

• Smoulokowski kinetics assumes each collision leads to a droplet aggregation.

• In fact only a tiny proportion of collisions are reactive

2P

P2

G

G

kslow=kfast/W

Function of energy barrier

Page 6: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

An Interaction Potential

• A plot showing energy to move a particle from an infinite distance to a given distance from a second particle.

• The pair of particles will try to find the optimum separation to minimize energy but can be blocked by a significant (>2-3 kT) energy barrier.

Page 7: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Van der Waals Attraction

-100

-50

0

0 20 40

Separation, nmV

A/k

T, J

h

ArVA 12

Hamaker constant~5e-21 J

• Always attractive

• Very short range

Page 8: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Surface Charge =0e-h

Page 9: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Effective Charge

0

2

4

6

8

10

12

0 10 20 30 40Distance

Pot

entia

l

Low ionic strength=long range

=0e-h

High ionic strength=short range

Effective charge at distance h

Surface charge

Distance from surface

Reciprocal Debye length – increases with ionic strength

Page 10: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Electrostatic Repulsion

• Repulsive or attractive depending on sign of charges

• Magnitude depends on magnitude of the charge

• Gets weaker with distance but reasonably long range

• Short range at high I

)1ln(2 khE ekrV

0

100

200

0 10 20

Separation /nm

VE/k

T, J

Page 11: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

-0.10

-0.08

-0.06

-0.04

-0.02

0.00

0.02

0.04

0.06

0.08

0.10

0 5 10 15 20

Separation

Inte

ract

ion

fre

e en

erg

y

I=0.3 I=0.4

I=0.5 I=0.6

• VDVLO=VVdW+Velectrostatic

• The height of the barrier increases with surface potential

• Its width increases with decreasing I

DVLO Theory

Page 12: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Steric Repulsion

Droplets approach each other

Protein layers overlap

Proteins repel each other mechanically & by osmotic dehydration

What happens when protein molecules on different droplets are reactive?

Page 13: Colloidal Aggregation FDSC400. Goals Aggregation rate Interaction potentials Electrostatic repulsion Van der Waals attraction DVLO theory Steric repulsion

Dispersed Systems-summary-

• Types of dispersed system• Surface tension• Surface active materials• Properties of emulsions• Mechanisms of emulsion destabilization

(stabilization)• Foams• Aggregation kinetics• DVLO theory and modifications