Two phases are in equilibrium when
μ1(T,P)=μ2(T,P) So
dμ1(T,P)=dμ2(T,P)
(∂T∂μ1)PdT+(∂P∂μ1)TdP=(∂T∂μ2)PdT+(∂P∂μ2)TdP Using Maxwell's relations
(∂T∂μ)P=−S
(∂P∂μ)T=V we obtain
−S1dT+V1dP=−S2dT+V2dP Finally
dTdP=V2−V1S2−S1 Since
TΔS=Q we also have
dTdP=T(V2−V1)Q
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