For the first step, since the state law is PV2=k, we can consider that P=V2k and P1V12=k=P2V22 both satisfy that equation, thus we calculate the work for these conditions as:
P1=20bar=2×106PaV1=0.05m3P2=V22P1V12=4P1=5bar=5×105PaV2=2V1=0.10m3W1ststep=−∫pdV=−∫V1V2kV2dVW1ststep=k[V1]V1V2=P1V12[V21−V11]W1ststep=P1V1[V2V1−1]W1ststep=(2×106Pa)(0.05m3)(0.10m30.05m3−1)W1ststep=(2×106)(0.05)(−21)Pa⋅m3(1000Pa⋅m31kJ)W1ststep=−50kJ
For the second step, we have to consider that the process happens with constant pressure, thus the work can be found as:
P1=P2=5bar=5×105PaV1=0.10m3V2=2V1=0.05m3W2ndstep=−∫pdV=−P1∫V1V2dVW2ndstep=−P1[V]V1V2=−P1(V2−V1)W2ndstep=−(5×105Pa)(0.05−0.10)m3W2ndstep=−(5×105)(−0.05)Pa⋅m3(1000Pa⋅m31kJ)W2ndstep=25kJ
For the third step, since the process occurs at constant volume (because the piston is locked in its position) there is no work done thus:
P1=5bar=5×105PaP2=20bar=2×106PaV2=V1=0.05m3W3rdstep=−∫pdV (since dV=0) W3rdstep=0kJ
The total work done is WT=W1ststep+W2ndstep+W3rdstep=(−50+25+0)kJ=−25kJ.
Reference:
- Sears, F. W., & Zemansky, M. W. (1973). University physics.
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