Blundell Thermal Physics · Problem 18.2

The third law

Physics — Statistical Mechanics · gibbs-enthalpy-third-law

Problem

Recall from eqn 16.26 that H=G−T(∂G∂T)p.(18.9)H = G - T\left(\frac{\partial G}{\partial T}\right)_p. \tag{18.9} Hence show that ΔG−ΔH=T(∂ΔG∂T)p,(18.10)\Delta G - \Delta H = T\left(\frac{\partial \Delta G}{\partial T}\right)_p, \tag{18.10} and explain what happens to these terms as the temperature T→0T \to 0.

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