Hence,as
|
(2.57) |
|
(2.58) |
|
(2.59) |
|
(2.60) |
Now,
|
(2.61) |
Now μ is defined as chemical potential.
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) |
