Step 1: Recall the fundamental thermodynamic relation.
For a closed system,
\[
dU = T dS - P dV
\]
Step 2: Identify the Maxwell relation.
From this relation, by using exact differential properties, the Maxwell relation becomes:
\[
\left(\frac{\partial P}{\partial T}\right)_V = \left(\frac{\partial S}{\partial V}\right)_T
\]
Step 3: Conclusion.
Thus, the correct Maxwell relation is given in option (B).
