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| $List-I$ | $List-II$ |
| $(P)$ Work done in the complete cyclic process | $(1)$ $R T_0 - 4 R T_0 \ln 2$ |
| $(Q)$ Change in the internal energy of the gas in the process $JK$ | $(2)$ $0$ |
| $(R)$ Heat given to the gas in the process $KL$ | $(3)$ $3 R T_0$ |
| $(S)$ Change in the internal energy of the gas in the process $MJ$ | $(4)$ $-2 R T_0 \ln 2$ |
| $(5)$ $-3 R T_0 \ln 2$ |
| Column-$I$ | Column-$II$ |
| $(A)$ $PV$ vs $V$ (Isothermal expansion) | $(P)$ $W$ > 0 |
| $(B)$ $P$ vs $T$ (Isochoric heating) | $(Q)$ $W$ < 0 |
| $(C)$ $P$ vs $V$ (Isobaric expansion) | $(R)$ $\Delta Q$ > 0 |
| $(D)$ $V$ vs $T$ (Isobaric compression) | $(S)$ $\Delta U$ > 0 |
| $(T)$ $\Delta U$ < 0 |
| Column $I$ | Column $II$ | Column $III$ |
|---|---|---|
| $(I)$ $W_{1-2} = \frac{1}{\gamma-1}(P_2V_2 - P_1V_1)$ | $(i)$ Isothermal | $(P)$ [Graph $P$] |
| $(II)$ $W_{1-2} = -P(V_2 - V_1)$ | (ii) Isochoric | $(Q)$ [Graph $Q$] |
| $(III)$ $W_{1-2} = 0$ | (iii) Isobaric | $(R)$ [Graph $R$] |
| $(IV)$ $W_{1-2} = -nRT \ln(\frac{V_2}{V_1})$ | (iv) Adiabatic | $(S)$ [Graph $S$] |
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