A thermodynamic system goes from states (i) P1, V to 2P1, V (ii) P, V1 to P, 2V1. Then work done in the two cases is
Zero, Zero
Zero, PV1
PV1, Zero
PV1, P1V1
(i) Case → Volume = constant ⇒∫PdV=0
(ii) Case →P= constant ⇒∫V12V1 PdV=P∫V12V1 dV=PV1