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ELECTROKINETIC PHENOMENA

Electrokinetic phenomena include Electrophoresis, electrosmosis, sedimentation potential and Streaming potential, whereby a potential is created when charged particles move with respect to a stationary liquid or particles move upon application of a potential. The phenomena are evidence that particles are charged. 

Electrophoresis:
When a dc electric field is applied to a dispersion, the particles move towards the electrode of a charge opposite to that on their surface. The counterions located inside their hydration shell are dragged along. The counterions in the diffuse layer outside the plane of shear will move towards the other electrode. This phenomenon is called electrophoresis. The rate of migration of particles is observed by means of an ultramicroscopic and is a function of the charge on particle. As mentioned earlier, the potential at the plane of shear is the Zeta potential. The sign and magnitude of zeta potential can be measured from a knowledge of the direction and rate of migration.

ζ =       ν  x  4πη  x (9 x 104)
E       ε

Where ν is the velocity of migration (cm/sec)
η = viscosity of the medium (poise), ε is the dielectric constant
E is potential gradient (volts/cm).
ζ  is in volts.
The expression v/E is known as mobility.

Sedimentation potential:
The reverse of electrophoresis, that is a potential is created when particles undergo sedimentation (against a stationary liquid).

Electrosmosis:
If a charged surface is immobile (e.g. a packed bed of particles), application of an electric field causes the counterions in the free water to move towards the opposite electrode, dragging the solvent with them. Thus the liquid moves relative to the stationary charged surface, and the phenomenon is known as electrosmosis. The pressure produced is the electroosmotic pressure. By determining the rate of flow of a liquid under standard conditions, Zeta potential can be measured.

Streaming potential
If the liquid is made to flow past a charged surface in a capillary tube by applying hydrostatic pressure, the displacement of the counterions in the free water produces a potential difference between the two ends of the tube or bed. This potential is known as Streaming Potential. Measuring this potential, Es, and knowing the applied pressure, P, we can obtain from zeta potential from the following equation:

ζ =   4πηκΕl
            εP

Where l = length of capillary, and κ is conductivity of liquid.