$A$ thermodynamic system goes from states $(i) \, P_1, V$ to $2P_1, V$ and $(ii) \, P, V$ to $P, 2V$. The work done in the two cases is:

  • A
    Zero,Zero
  • B
    Zero,$PV$
  • C
    $PV$,Zero
  • D
    $PV, P_1V$

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