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Chemistry · Ch 7 — Thermodynamics

Relationship between ΔG0 and Keq

7.11.2

Relationship between ΔG0 and Keq

In a reversible chemical equilibrium, the system stays in perfect equilibrium with its surroundings at every instant, and the reaction can proceed in both the forward and reverse directions SIMULTANEOUSLY, so that a dynamic equilibrium is set up. For both directions to keep proceeding with a decrease in free energy (as spontaneity would seem to demand) is only possible if, right AT equilibrium, the system's free energy sits at a genuine MINIMUM.

For a general equilibrium reaction A+B⇌C+DA+B\rightleftharpoons C+D, the free energy change in any (non-equilibrium) state, ΔG\Delta G, is related to the standard free energy change, ΔG0\Delta G^0, by:

ΔG=ΔG0+RTln⁡Q(7.39)\Delta G = \Delta G^0+RT\ln Q \qquad (7.39)

where QQ is the reaction quotient -- the ratio of product concentrations to reactant concentrations under whatever (non-equilibrium) conditions currently apply.

When the system reaches equilibrium, there is no further free energy change (ΔG=0\Delta G=0), and QQ becomes equal to the equilibrium constant KeqK_{eq}. Equation (7.39) then reduces to:

ΔG0=−RTln⁡Keq\Delta G^0 = -RT\ln K_{eq}

known as the Van't Hoff equation, more commonly written using base-10 logarithms as:

ΔG0=−2.303 RTlog⁡Keq(7.40)\Delta G^0 = -2.303\,RT\log K_{eq} \qquad (7.40)

We also know from (7.36) that ΔG0=ΔH0−TΔS0\Delta G^0=\Delta H^0-T\Delta S^0, so all three quantities are linked: ΔG0=ΔH0−TΔS0=−RTln⁡Keq\Delta G^0=\Delta H^0-T\Delta S^0=-RT\ln K_{eq}. …

Misc 7.9Problem 7.9 -- $\Delta G^0$ for ozone formation from $K_p$

Worked out. 32O2⇌O3(g)\tfrac{3}{2}O_2\rightleftharpoons O_3(g) at T=298T=298 K, Kp=2.47×10−29K_p=2.47\times10^{-29}, R=8.314R=8.314 JK−1^{-1}mol−1^{-1}. ΔG0=−2.303RTlog⁡Kp=−2.303(8.314)(298)log⁡(2.47×10−29)=163,229\Delta G^0=-2.303RT\log K_p=-2.303(8.314)(298)\log(2.47\times10^{-29})=163{,}229 J mol−1=163.229^{-1}=163.229 kJ mol−1^{-1}. …