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An ideal gas exists in a state with pressure $$P_0$$, volume $$V_0$$. It is isothermally expanded to 4 times of its initial volume $$(V_0)$$, then isobarically compressed to its original volume. Finally the system is heated isochorically to bring it to its initial state. The amount of heat exchanged in this process is:
Initial state:
$$(P_0,V_0)$$For one complete cycle,
$$ΔU=0$$So net heat exchanged equals net work done:
$$Q=W$$
Now calculate work in each process.
For isothermal process,
$$W_1=nRT\ln\frac{4V_0}{V_0}$$
Since initially
$$nRT=P_0V_0$$
So
$$W_1=P_0V_0\ln4$$
After isothermal expansion pressure becomes
$$P=\frac{P_0V_0}{4V_0}=\frac{P_0}{4}$$
Compression occurs at constant pressure $$\frac{P_0}{4}\ from\ 4V_0\ to\ V_0$$.
Work done:
$$W_2=P\Delta V=\frac{P_0}{4}(V_0-4V_0)$$$$=-\frac{3}{4}P_0V_0$$$$W_3=0$$
Net work:
$$W=P_0V_0\ln4-\frac{3}{4}P_0V_0$$
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