2. Understanding Corrosion | |
2.5.1 Relationship between 'Free Energy' and 'Equilibrium Constant' |
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The contribution made by one mole of any constituent, A, to the total free energy, G, of the mixture is GA, which may be represented by
GA = GAo RT ln(aA) |
where aA = activity of the substance, T = absolute temperature, and R = gas constant. |
From the Gibbs-Helmholtz equation:
G = H - TS
Substituting H from the First Law of Thermodynamics
G = U + PV - TS
Differentiating:
dG = dV + PdV + VdP - TdS - SdT
But,
dV = qrev - PdV and qrev = TdS
So,
dG = TdS - PdV + PdV + VdP - TdS - SdT
i.e., dG = VdP - SdT
At constant pressure, this equation becomes:
and at constant temperature:
dG = VdP
However, for ideal gas equation for 1 mole of reaction is
pV = RT |
V = RT/p |
Integration between the limits gives
If G'A is taken to refer for standard conditions, it becomes GAo.
(1)
If activities are concerned instead of pressure, then
Applying DG for the reaction: aA + bB cC + dD gives
Expressing GC, GD, GA and GB as shown in (1) above, we get
So, for 1 mole forward reaction,
(2)
and at equilibrium, DG = 0
Equation (2) may be written as
The equations linking DG and K are referred to as VanHoff's Isotherms.
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