Please help show that ((delT)/(delP))_S = (ValphaT)/C_P(TP)S=VαTCP?

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1 Answer
Jan 25, 2017

Okay, considering that ((delT)/(delP))_S(TP)S contains SS, TT, and PP, I would start from S = S(T,P)S=S(T,P) and take the total derivative:

dS = ((delS)/(delT))_PdT + ((delS)/(delP))_TdPdS=(ST)PdT+(SP)TdP " "" "bb((1)) (1)

Now, if we divide by delPP at a constant SS, we'd get:

cancel(((delS)/(delP))_S)^(0) = ((delS)/(delT))_P((delT)/(delP))_S + ((delS)/(delP))_Tcancel(((delP)/(delP))_S)^(1)

" "" "bb((2))

since a constant S forces a derivative of S with respect to any variable to go to 0, and (dP)/(dP) = 1 no matter what else is held constant.

From this question, we can refer back and recall that

((delS)/(delT))_P = 1/T ((delH)/(delP))_T = C_P/T.

bb((3))

Now we need to figure out what ((delS)/(delP))_T is.

The bottom of the derivative shows T and P, which are the natural variables of the Gibbs' free energy, so from the Maxwell relation:

dG = -SdT + VdP,

we can either recall the cyclic relation ((delS)/(delP))_T = -((delV)/(delT))_P, or rederive it. Again, from the total derivative of G(T,P):

dG = ((delG)/(delT))_PdT + ((delG)/(delP))_TdP,

showing that -S = ((delG)/(delT))_P and V = ((delG)/(delP))_T. Since the order of second partial differentiation doesn't matter,

((del^2G)/(delPdelT))_(P,T) = ((del^2G)/(delTdelP))_(T,P),

meaning that

-((delS)/(delP))_T = ((delV)/(delT))_P. " "" "bb((4))

Therefore, from bb((2)), subtract over ((delS)/(delP))_T, plug in bb((3)) and bb((4)), and we have:

((delV)/(delT))_P = C_P/T((delT)/(delP))_S

=> ((delT)/(delP))_S = T/C_P ((delV)/(delT))_P

Finally, recall that alpha = 1/V((delV)/(delT))_P, so that we have:

=> color(blue)(((delT)/(delP))_S = (ValphaT)/C_P)