Using Maxwell's relations, derive the first and second energy equations.
Maxwell's relations are derived from the thermodynamic potentials and are fundamental in thermodynamics and statistical mechanics. To derive the first and second energy equations, we utilize the thermodynamic potentials and the differential forms of internal energy \( U \), enthalpy \( H \), Helmholtz free energy \( F \), and Gibbs free energy \( G \).
### First Energy Equation
The internal energy \( U \) is expressed as:
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