371267 Amongst the two paths that may be taken by a gas to go from a state \(A\) to a state \(C\), in process \(AB\) (as shown in figure), \(360\;J\) of heat is added to the system. In process \(BC,140\;J\) of heat is added to the system. The heat absorbed by the system in the process \(AC\) will be

371268 One mole of an ideal gas is taken from \(A\) to \(B\), from \(B\) to \(C\) and then back to \(A\). The variation of its volume with temperature for that change is as shown.
Its pressure at \(A\) is \({P_0}\), volume is \({V_0}\). Then, the internal energy

371269 Two moles of an ideal monoatomic gas are taken through a cycle \(A B C A\) as shown in the \(P T\) diagram in figure. During the process \(A B\), pressure and temperature of the gas vary such that \(P T=\) constant. If \(T_{0}=300 {~K}\), and the heat released by the gas in the process \(A B\) (in \(kJ\)).
\((R = 8.3\,J/mo{l^{ - K}})\)

371270 A real gas within a closed chamber at \({27^{\circ} {C}, P\left({~N} / {m}^{2}\right)}\) undergoes the cyclic process as shown in figure. The gas obeys \({P V^{3}=R T}\) equation for the path \({A}\) to \({B}\). The net work done in the complete cycle is
\(({\text{assuming }}\,R = 8\,J/mol\,K)\)

371267 Amongst the two paths that may be taken by a gas to go from a state \(A\) to a state \(C\), in process \(AB\) (as shown in figure), \(360\;J\) of heat is added to the system. In process \(BC,140\;J\) of heat is added to the system. The heat absorbed by the system in the process \(AC\) will be

371268 One mole of an ideal gas is taken from \(A\) to \(B\), from \(B\) to \(C\) and then back to \(A\). The variation of its volume with temperature for that change is as shown.
Its pressure at \(A\) is \({P_0}\), volume is \({V_0}\). Then, the internal energy

371269 Two moles of an ideal monoatomic gas are taken through a cycle \(A B C A\) as shown in the \(P T\) diagram in figure. During the process \(A B\), pressure and temperature of the gas vary such that \(P T=\) constant. If \(T_{0}=300 {~K}\), and the heat released by the gas in the process \(A B\) (in \(kJ\)).
\((R = 8.3\,J/mo{l^{ - K}})\)

371270 A real gas within a closed chamber at \({27^{\circ} {C}, P\left({~N} / {m}^{2}\right)}\) undergoes the cyclic process as shown in figure. The gas obeys \({P V^{3}=R T}\) equation for the path \({A}\) to \({B}\). The net work done in the complete cycle is
\(({\text{assuming }}\,R = 8\,J/mol\,K)\)

371267 Amongst the two paths that may be taken by a gas to go from a state \(A\) to a state \(C\), in process \(AB\) (as shown in figure), \(360\;J\) of heat is added to the system. In process \(BC,140\;J\) of heat is added to the system. The heat absorbed by the system in the process \(AC\) will be

371268 One mole of an ideal gas is taken from \(A\) to \(B\), from \(B\) to \(C\) and then back to \(A\). The variation of its volume with temperature for that change is as shown.
Its pressure at \(A\) is \({P_0}\), volume is \({V_0}\). Then, the internal energy

371269 Two moles of an ideal monoatomic gas are taken through a cycle \(A B C A\) as shown in the \(P T\) diagram in figure. During the process \(A B\), pressure and temperature of the gas vary such that \(P T=\) constant. If \(T_{0}=300 {~K}\), and the heat released by the gas in the process \(A B\) (in \(kJ\)).
\((R = 8.3\,J/mo{l^{ - K}})\)

371270 A real gas within a closed chamber at \({27^{\circ} {C}, P\left({~N} / {m}^{2}\right)}\) undergoes the cyclic process as shown in figure. The gas obeys \({P V^{3}=R T}\) equation for the path \({A}\) to \({B}\). The net work done in the complete cycle is
\(({\text{assuming }}\,R = 8\,J/mol\,K)\)

371267 Amongst the two paths that may be taken by a gas to go from a state \(A\) to a state \(C\), in process \(AB\) (as shown in figure), \(360\;J\) of heat is added to the system. In process \(BC,140\;J\) of heat is added to the system. The heat absorbed by the system in the process \(AC\) will be

371268 One mole of an ideal gas is taken from \(A\) to \(B\), from \(B\) to \(C\) and then back to \(A\). The variation of its volume with temperature for that change is as shown.
Its pressure at \(A\) is \({P_0}\), volume is \({V_0}\). Then, the internal energy

371269 Two moles of an ideal monoatomic gas are taken through a cycle \(A B C A\) as shown in the \(P T\) diagram in figure. During the process \(A B\), pressure and temperature of the gas vary such that \(P T=\) constant. If \(T_{0}=300 {~K}\), and the heat released by the gas in the process \(A B\) (in \(kJ\)).
\((R = 8.3\,J/mo{l^{ - K}})\)

371270 A real gas within a closed chamber at \({27^{\circ} {C}, P\left({~N} / {m}^{2}\right)}\) undergoes the cyclic process as shown in figure. The gas obeys \({P V^{3}=R T}\) equation for the path \({A}\) to \({B}\). The net work done in the complete cycle is
\(({\text{assuming }}\,R = 8\,J/mol\,K)\)