Work done in a thermodynamic process is given by ∫pdV\int pdV∫pdV
pV=cp=c/VpV=c\\p=c/VpV=cp=c/V
substituting this into the work done formula we get
Work done = ∫cVdV\smallint \frac{c}{V}dV∫VcdV
Integrating this with limits V1V_1V1 to V2V_2V2
Work done =[clnV]V1V2[c\ln V]^{V_2}_{V_1}[clnV]V1V2 =clnV2V1c\ln\frac{V_2}{V_1}clnV1V2
as we are given pV=c which means p1V1=c
substituting the value of c , we get
Work done = p1V1lnV2V1p_1V_1\ln{\frac{V_2}{V_1}}p1V1lnV1V2
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