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