The thermodynamic derivation of the distribution law is based upon he principle that if there are two phases in equilibrium (i.e. two immiscible solvents containing the same solute dissolved in them), the chemical potential of a substance present in them must be same in both the phases.
The chemical potential of a substance in a solution given by
Where 'm' is the standard chemical potential and ‘a’ is the activity of the substance (solute) in the solution.
Thus for the solute in liquid A, we have
Similarly for the solute in liquid B we have
But as already stated, since the liquids A and B are in equilibrium,
Further at a given temperature, 'mA' and 'mB' are constant for given substance in the particular solvents. Hence at constant temperature, we have from equation
and therefore
Which is the original form of the distribution law.
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