Using Maxwell’s relations, deduce first and second TdS equations
Answer
According to thermodynamics
We can express entropy in terms of any two of PVT. Let us first express entropy as a function of V and T
"d S=\\left(\\frac{\\partial S}{\\partial V}\\right)_{T} d V+\\left(\\frac{\\partial S}{\\partial T}\\right)_{V} d T."
As
"T d S=T\\left(\\frac{\\partial S}{\\partial V}\\right)_{T} d V+T\\left(\\frac{\\partial S}{\\partial T}\\right)_{V} d T."
Now using maxwell equation
"\\left(\\frac{\\partial S}{\\partial V}\\right)_{T}=\\left(\\frac{\\partial P}{\\partial T}\\right)_{V}" Using Tds=dU
"T\\left(\\frac{\\partial S}{\\partial T}\\right)_{V}=\\left(\\frac{\\partial U}{\\partial T}\\right)_{V}=C_{V}"
This is the first of the TdS equations.
Now let us express entropy as a function of P and T
"d S=\\left(\\frac{\\partial S}{\\partial P}\\right)_{T} d P+\\left(\\frac{\\partial S}{\\partial T}\\right)_{P} d T."
"T d S=T\\left(\\frac{\\partial S}{\\partial P}\\right)_{T} d P+T\\left(\\frac{\\partial S}{\\partial T}\\right)_{P} d T."
Using maxwell equation
"\\left(\\frac{\\partial S}{\\partial P}\\right)_{T}=-\\left(\\frac{\\partial V}{\\partial T}\\right)_{P}"
We know Tds=dU
"T\\left(\\frac{\\partial S}{\\partial T}\\right)_{P}=\\left(\\frac{\\partial H}{\\partial T}\\right)_{P}=C_{P}"
So
"T d S=-T\\left(\\frac{\\partial V}{\\partial T}\\right)_{P} d P+C_{P} d T."
This is the first of the TdS equations.
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