| 2. Understanding Corrosion | |
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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
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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 |
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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
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Applying DG for the reaction:
aA
+ bB
cC
+ dD gives
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Expressing GC, GD, GA and GB as shown in (1) above, we get
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So, for 1 mole forward reaction,
(2)
and at equilibrium, DG = 0

Equation (2) may be written as
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The equations linking DG and K are referred to as VanHoff's Isotherms.
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