Thermodynamics

\({{\Delta {G_{System}}} \over {\Delta {S_{Total}}}} = - T\) (at constant P)

\(K = {{\Delta H^\circ - T\Delta S^\circ } \over {RT}}\)

\(K = {e^{ - \Delta G^\circ /RT}}\)

For isothermal process \({w_{reversible}} = - nRT\ln {{{V_f}} \over {{V_i}}}\)