Step 1. Understanding the Slopes in the log P vs. log V Diagram:
Process A has a slope of \( \tan^{-1} \gamma \), where \( \gamma = \frac{C_P}{C_V} \), indicating an adiabatic process (since \( PV^\gamma = \text{constant} \)). Process B has a slope of \( 45^\circ \) or \( \tan^{-1} 1 \), suggesting that it is an isothermal process (since \( PV = \text{constant} \)).
Step 2. Using Heat Capacities for Adiabatic and Isothermal Processes:
For an adiabatic process (\( PV^\gamma = \text{constant} \)), the heat capacity \( C_A \) is effectively zero because no heat exchange occurs (\( dQ = 0 \) for adiabatic). For an isothermal process (\( PV = \text{constant} \)), the heat capacity \( C_B \) tends to infinity because any heat added is used to perform work without changing temperature.
Conclusion:
Therefore, the correct statement is:
\[ C_A = 0 \quad \text{and} \quad C_B = \infty \]
List-I | List-II | ||
(A) | Isothermal process | (I) | No heat exchange |
(B) | Isochoric process | (II) | Carried out at constant temperature |
(C) | Isobaric process | (III) | Carried out at constant volume |
(D) | Adiabatic process | (IV) | Carried out at constant pressure |