1. Physical Pharmacy 2
COLLOID: ELECTRICAL DOUBLE LAYER Kausar Ahmad
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2. Contents Electrical Double Layer theories
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Contents
Electrical Double Layer theories
Repulsive effect of Electrical Double Layer
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3. Physical Pharmacy 2
HELMHOLTZ EDL
Helmholtz in 1879 introduced the concept of the electrical double layer.
Charge on the particles of a lyophobic colloid due to unequal distribution of ions at the particle-water interface.
If ions of one charge were closely bound to the particle, ions of opposite charge would line up parallel to them, forming a double layer of charges
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4. GOUY DIFFUSE DOUBLE LAYER
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GOUY DIFFUSE DOUBLE LAYER
Double layer is diffused
outer ionic layer having an electric density falling off according to an exponential law.
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5. STERN DIFFUSE DOUBLE LAYER
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STERN DIFFUSE DOUBLE LAYER
Stern compromised Helmholtz and Gouy - the double layer is in two parts:
Helmholtz layer
one layer approximately a single ion in thickness, remains fixed to the interfacial surface. In this layer, there is a sharp drop of potential.
2. Gouy layer
this layer extends some distance into the liquid dispersing phase and is diffuse, with a gradual fall in potential into the bulk of the liquid.
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6. Physical Pharmacy 2
ELECTRIC DOUBLE LAYER
is a region of molecular dimension at the boundary of two substances across which an electrical field exists.
The substances must each contain electrically charged particles, such as electrons, ions, or molecules with a separation of electrical charges (polar molecules).
In the EDL, oppositely charged particles attract each other and tend to collect at the surface of each substance but remain separated from one another by the finite size of each particle or by neutral molecules that surround the charged particles.
The electrostatic attraction between the two opposite and separated charges causes an electrical field to be established across the interface.
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7. ELECTRICAL DOUBLE LAYER
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ELECTRICAL DOUBLE LAYER
The double layer is formed in order to neutralize the charged surface and, in turn, causes an electrokinetic potential between the surface and any point in the mass of the suspending liquid. This voltage difference is on the order of millivolts and is referred to as the surface potential. The magnitude of the surface potential is related to the surface charge and the thickness of the double layer. As we leave the surface, the potential drops off roughly linearly in the Stern layer and then exponentially through the diffuse layer, approaching zero at the imaginary boundary of the double layer. The potential curve is useful because it indicates the strength of the electrical force between particles and the distance at which this force comes into play. A charged particle will move with a fixed velocity in a voltage field. This phenomenon is called electrophoresis. The particle’s mobility is related to the dielectric constant and viscosity of the suspending liquid and to the electrical potential at the boundary between the moving particle and the liquid. This boundary is called the slip plane and is usually defined as the point where the Stern layer and the diffuse layer meet. The relationship between zeta potential and surface potential depends on the level of ions in the solution.The figure above represents the change in charge density through the diffuse layer. One shows considered to be rigidly attached to the colloid, while the diffuse layer is not. As a result, the electrical potential at this junction is related to the mobility of the particle and is called the zeta potential. Although zeta potential is an intermediate value, it is sometimes considered to be more significant than surface potential as far as electrostatic repusion is concerned.
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8. REPULSIVE EFFECT OF EDL
Physical Pharmacy 2
REPULSIVE EFFECT OF EDL
Repulsive effect from the EDL is responsible for stability.
Repulsive potential energy is a function of (from Verwey and Overbeek):
Distance between droplets
The reciprocal of the effective radius of the double layer
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9. REPULSIVE POTENTIAL ENERGY
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REPULSIVE POTENTIAL ENERGY
From Verwey and Overbeek
VR = 4.62 x 10-6 (r/2) e-kHo
VR Repulsive potential energy
r Particle radius
 Valence of counter ions
Ho distance between two particles
 = (ez/2 – 1) / (ez/2 + 1); Z = ueo/kT, o is the EDL potential
 Boltzmann constant
Exercise: Predict VR in the presence of high valency counter ions
Exercise: Predict VR when distance between particles is small
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10. ATTRACTIVE POTENTIAL ENERGY
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ATTRACTIVE POTENTIAL ENERGY
A small attractive Van der Waals force operating between the droplets, can be given by:
VA = -Ar/12H0
A is a constant depending on the polarisability of the molecules of which the droplet is composed and is known as the Hamaker constant; A ca J to J.
Exercise: what happen if you have big ‘r’?
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11. DLVO THEORY VT = VA + VR From Derjaguin, Landau, Verwey and Overbeek
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DLVO THEORY
From Derjaguin, Landau, Verwey and Overbeek
Describes the stability of hydrophobic suspension
Electrostatic repulsive potential energy, VR, and the attractive potential energy, VA, gives the total potential energy of interaction:
VT = VA + VR
The forces on colloidal particles in a dispersion are due to electrostatic repulsion and London-type Van der Waals forces
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12. ENERGY OF INTERACTION & DISTANCE BETWEEN PARTICLES
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ENERGY OF INTERACTION & DISTANCE BETWEEN PARTICLES
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13. INTERACTION POTENTIALS
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INTERACTION POTENTIALS
polystyrene sulfate spheres in deionized water at 25oC.
Curves are labelled by the spheres' radii.
Exercise: Compare the interaction potentials of big particles to small particles when the distance that separates them is the same.
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14. Physical Pharmacy 2
REFERENCES
RJ Hunter, Foundations of Colloid Science Volume 2, Clarendon Press Oxford (1989)
…and as indicated on slides…‏
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