| List-$I$ | List-$II$ |
| $A$. At constant volume the change in internal energy of a system | $I$. $W = -2.303 nRT \log \frac{V_f}{V_i}$ |
| $B$. Isothermal irreversible change | $II$. $W_{adiabatic} = \Delta U$ |
| $C$. Isothermal reversible change | $III$. $q_V = \Delta U$ |
| $D$. Adiabatic change | $IV$. $W = -p_{ex} (V_f - V_i)$ |
| $V$. $\Delta U = \Delta H - \Delta nRT$ |
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| List-$I$ | List-$II$ |
|---|---|
| $(A) \Delta U = W_{ad}$ | $I.$ Isothermal reversible expansion |
| $(B) \Delta U = q - W$ | $II.$ Wall is adiabatic |
| $(C) \Delta U = -q$ | $III.$ Thermally conducting walls |
| $(D) \Delta U = 0$ | $IV.$ Isolated system |
| $V.$ Closed system |
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