5. Colloidal interaction and surface forces

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Last updated 6:33 AM on 5/26/24
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21 Terms

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Stability of colloidal dispersions

  •  Almost always thermodynamically unstable systems

  •  Kinetics and interaction determine stability

  •  Time is important – stability from minutes to 100s of years (for example Italian salad dressing is short)

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Colloidal interactions

Interactions between colloidal particles → forces between particles

  • Attraction (if it comes close enough) and repulsion

  • Range of interaction (how close can two particles get before anything happens) is important!

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Flocculation

a process where a solute comes out of solution in the form of floccules or flakes

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van der Waals interactions

• Caused by molecular dipole interactions (impermanent, permanent and induced)

• Comparably long-ranged, but weak at long distances.

• Strong at short distances (smooth surfaces tend to get closer to each other) 

Attractive force between surfaces is always present 

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Van der Waals force between surfaces

It decays were fast with larger distances 

A=Hamaker constant (J)

L=separation between surfaces

P=attractive pressure (N/m2)

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Electrostatic repulsion

• Caused by charge at surfaces 

• In low dielectric media → coulomb interaction (continuous phase typically air and oil/apolar solvents)

– Charge level could be very high and operating distance very long

– Important in clouds (thunder)

– Sparks

• In dielectric media (polar solvent, typically water) a diffuse counter-ion cloud is formed

– Neutralising the long range character of the coulomb forces.

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Electrical field and charge densities

• A charged surface gives rise to an electric potential in a dielectric medium (such as water)

• The electric potential decays from the surface – depends on the charge density in the solution (i.e. ionic strength)

• Ions in solution ”screen” the charge of the surface

• Creation of the double layer (one charge on the surface and another a bit further away from surface (diffused ion cloud of counter ion, not every ion on surface has it own counter ion))



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Double layer

Counter-ions are attracted to the charged surface and a “double layer” is formed. The counter ion concentration decreases with distance from the surface

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Debye-Hückel length

By assuming symmetrical electrolytes we obtain the Debye-Hückel screening length


Higher charge (valence)→ shorter Debye-Huckel length 

Increasing concentration → shorter Debye-Huckel length 

LD=Debye-Huckel length 

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Electric potential

• Can be interpreted as the thickness of the electric double layer →  the range of electrostatic repulsion

• Depends strongly on valence and also on concentration


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What happens when two layer of different surface overlap?

Higher osmotic pressure → repulsion between the surfaces → solvent goes in

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Electrostatic repulsion

• Osmotic repulsion between overlapping clouds of counter ions (double layers)

• Resulting pressure:

• Range of the force depends on the thickness of the double layer (electric potential)

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DLVO theory

• van der Waals interaction dominates at very short distances → primary minimum

• van der Waals interaction dominates at long distances → secondary minimum

• The electrostatic repulsion may dominate at intermediate distances. This causes the electrostatic repulsive barrier.

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Example of Loss of electrostatic repulsion (salt water)

The high ionic strength in the ocean causes a loss of repulsion between particles (higher ionic strength —> reduce thickness of double layer). The particles gradually flocculate and as size increases they sediment out of dispersion.

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Steric repulsion between macromolecules

 • Osmotic repulsion between protruding (utstickande )chains of adsorbed macromolecules.

 • Caused by adsorbed (stuck to the surface) macromolecules

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Steric repulsion between macromolecules requires:

 • Adsorption of the macromolecule

 • Sufficient coverage of the interface

 • High solubility of the macromolecule (better than θ solvent)

 • Larger polymer → more efficient

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High and low solubility of macromolecule

Low solubility → try to get away from water

High solubility → protein will stretch out

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Bridging (attraction)

 • Partial coverage of surfaces can lead to the formation of macromolecular bridges between the surfaces.

 • Attractive (destabilizing) force


<p>&nbsp;• <mark data-color="yellow">Partial coverage of surfaces </mark>can lead to the formation of macromolecular bridges between the surfaces.</p><p>&nbsp;• Attractive (destabilizing) force</p><p></p>
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Depletion (attraction)

 • Caused by non-adsorbing polymers → no or low affinity for surface

 • Polymers avoid contact with surfaces

 • As polymers are depleted → osmotic gradient is created

 • Occurs at intermediate polymer concentrations and large polymer size (high molar mass)

 • Examples in aqueous dispersions are, dextran, PEG and other non-ionic polymers

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Hydration forces (repulsion)

 • Hydrated surfactants at the interface

 • Caused by the interaction between the emulsifier layer and the aqueous phase

 • Empirically described force



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Hydrophobic interaction (attraction)

 • Between hydrophobic macroscopic surfaces

 • Experimentally observed but, fundamentally, poorly understood force