Show that the following equation holds, relating the Helmholtz free energy to the constant-volume heat capacity of a material.
\left\lgroup\frac{\partial^2A}{\partial T^2} \right\rgroup _v=-\left\lgroup\frac{\partial S}{\partial T} \right\rgroup_v=-\left\lgroup\frac{c_v}{T} \right\rgroup