Concept:
Thermodynamic properties are defined by partial derivatives of state functions (U, H, G, etc.). Understanding these definitions is key to applying the First and Second Laws of Thermodynamics.
Step 1: Match A (Entropy).
For a reversible process, Entropy (S) (A) is defined by the Clausius inequality/equality as \( dS = \delta q / T \) (III).
Step 2: Match B and C (Heat Capacities).
\(C_P\) (B) is the heat capacity at constant pressure, defined as the rate of change of enthalpy with temperature: \( (\partial H / \partial T)_P \) (IV). \(C_V\) (C) is at constant volume, defined as the change in internal energy: \( (\partial U / \partial T)_V \) (I).
Step 3: Match D (Joule-Thomson).
The Joule-Thomson coefficient ($\mu_{JT}$) (D) describes the temperature change of a gas during an isenthalpic expansion: \( (\partial T / \partial P)_H \) (II).