Callen H.B - Thermodynamics And An Introduction To Thermostatistics · Problem 8.2-2

FIRST-ORDER PHASE TRANSITIONS

Physics — Statistical Mechanics · helmholtz-second-derivative-identity

Problem

Prove that (∂2F∂V2)T=∂2U∂S2∂2U∂V2−(∂2U∂S ∂V)2∂2U∂S2\left(\frac{\partial^2 F}{\partial V^2}\right)_T = \frac{\dfrac{\partial^2 U}{\partial S^2}\dfrac{\partial^2 U}{\partial V^2} - \left(\dfrac{\partial^2 U}{\partial S\,\partial V}\right)^2}{\dfrac{\partial^2 U}{\partial S^2}} Hint: Note that (∂2F/∂V2)T=−(∂P/∂V)T(\partial^2 F/\partial V^2)_T = -(\partial P/\partial V)_T, and consider PP formally to be a function of SS and VV.

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