$H _{2} O ( l ) \underset{0^{\circ} C , 1 \text{bar} }{\rightleftharpoons} H _{2} O ( s )$
for equilibrium at constant pressure and temperature.
$G = A + PV$
$d G = d A + PdV + VdP$
At constant $T$ and $P$ we obtain
$(\partial G )_{ T , P }=0$
for infinitesimal change
$(\Delta G )_{ T , P }>0$