A thermodynamic system goes from states $(i)\,\,{P_1}, V$ to $2{P_1}, V\, (ii)\, P, V$ to $P, 2V.$ Then work done in the two cases is
  • A
    Zero, Zero
  • BZero, $P{V_1}$
  • C$P{V_1}$, Zero
  • D$P{V_1},\;{P_1}{V_1}$
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