The Gibbs-Helmholtz equation is represented by:
1
\(\Delta G = \Delta H + T \left(\dfrac{\partial \Delta H}{\partial T}\right)_p\)
2
\(\Delta G = \Delta H - T \left(\dfrac{\partial \Delta G}{\partial T}\right)_p\)
3
\(\Delta G = \Delta H + T \left(\dfrac{\partial \Delta G}{\partial T}\right)_p\)
4
\(\Delta H = \Delta G + T \left(\dfrac{\partial \Delta G}{\partial T}\right)_p\)