An ideal gas exists in a state with pressure $P_0$, volume $V_0$. It is isothermally expanded to $4$ times 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

  • A
    $P_0 V_0(2 \ln 2 - 0.75)$
  • B
    $P_0 V_0(\ln 2 - 0.75)$
  • C
    $P_0 V_0(\ln 2 - 0.25)$
  • D
    $P_0 V_0(2 \ln 2 - 0.25)$

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