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{c}

Equality of mixed derivatives of $dG=-S\,dT+V\,dP$ gives
$$
\left(\frac{\partial S}{\partial P}\right)_T
=-\left(\frac{\partial V}{\partial T}\right)_P.
$$


Gibbs free-energy Maxwell relation

Past exam of the mathematics course of the University of Cambridge / 2015 / ii / Paper 3 / 33C / b / ii / Solution

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Past exam of the quantum condensed matter course of the University of Cambridge / 2004 / Section B / B7 / a / Solution

Gibbs free-energy Maxwell relation

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Gibbs free-energy Maxwell relation

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