Derive the following Maxwell relation: $\left(\frac{\partial V}{\partial T}\right)_P = -\left(\frac{\partial S}{\partial P}\right)_T$, starting from thermodynamic functions --i.e., functions of the form: d$U = TdS - PdV$. Show all steps clearly.
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Mathematically, this can be written as: dU = dQ - dW Show more…
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