Module 2 : Phase Transitions

Lecture 4 : Mixture of variable composition

Hence,as

(2.57)


(2.58)


(2.59)


(2.60)

Now,


(2.61)

Now μ is defined as chemical potential.

Gibbs-Duhem Equation

Let us consider a homogeneous phase of a multi-component system for which


(2.62)

If the phase is enlarged in size, U, S and V will increase in size, while T, p and μ will remain the same. Thus,


(2.63)

Let the system be enlarged to k times the original size.

∴ ΔU = kU - U = (k-1)U

(2.64a)


ΔS = kS - S = (k-1)S

(2.64b)


ΔV = kV - V = (k-1)V

(2.64c)


Δni = kni = ni = (k-1)ni

(2.64d)

Substituting Eqs. (2.64a-d) in Eq. (2.63), we get

(2.65)


(2.66)


(2.67)


(2.68)