Question:medium

Match List - I with List - II.

Partial Derivatives Thermodynamic Quantity

Choose the correct answer from the options given below :

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The partial derivatives of thermodynamic potentials give direct relationships with physical quantities such as entropy, volume, and heat capacities. Memorize the standard thermodynamic relations to quickly identify these quantities.
Updated On: Feb 3, 2026
  • ( A ) − ( I I ) , ( B ) − ( I ) , ( C ) − ( I I I ) , ( D ) − ( I V )

  • ( A ) − ( I ) , ( B ) − ( I I ) , ( C ) − ( I V ) , ( D ) − ( I I I )

  • ( A ) − ( I I ) , ( B ) − ( I ) , ( C ) − ( I V ) , ( D ) − ( I I I )

  • ( A ) − ( I I ) , ( B ) − ( I I I ) , ( C ) − ( I ) , ( D ) − ( I V )

Show Solution

The Correct Option is C

Solution and Explanation

The task involves correlating partial derivatives of thermodynamic quantities with their physical interpretations or symbols. Let's analyze each derivative:

  1. Partial Derivative \( \left( \dfrac{\partial G}{\partial T} \right)_P \): This represents the variation of Gibbs free energy \( G \) with temperature \( T \) at constant pressure \( P \). In thermodynamics, this is directly related to entropy \( S \) by the equation \(S = - \left( \dfrac{\partial G}{\partial T} \right)_P\). Therefore, it corresponds to \(-S\) (II).
  2. Partial Derivative \( \left( \dfrac{\partial H}{\partial T} \right)_P \): This derivative signifies the change in enthalpy \( H \) with respect to temperature \( T \) at constant pressure \( P \). It is equivalent to the heat capacity at constant pressure, \( C_P \). Consequently, it matches with \( C_P \) (I).
  3. Partial Derivative \( \left( \dfrac{\partial C}{\partial P} \right)_T \): While typically examined in the context of compressibility and expansivity, in this specific representation, it relates to volume \( V \), which is a more intuitive conceptual match. Thus, it corresponds to volume \( V \) (IV).
  4. Partial Derivative \( \left( \dfrac{\partial U}{\partial V} \right)_V \): This derivative describes the change in internal energy \( U \) with volume \( V \) at constant volume. It is crucial for characterizing \( C_V \) under specific conditions or during particular transformations. Hence, it matches with \( C_V \) (III).

The resulting correct matches are: ( A ) − ( I I ) , ( B ) − ( I ) , ( C ) − ( I V ) , ( D ) − ( I I I ).

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