d d T ( Δ r G T 0 T ) = − Δ r H T 0 T 2 {\displaystyle {\frac {\mathrm {d} }{\mathrm {d} T}}\left({\frac {\Delta _{r}G_{T}^{0}}{T}}\right)=-{\frac {\Delta _{r}H_{T}^{0}}{T^{2}}}}
