Van der Waals equation of state for one mole of a real gas is
( P + a V m 2 ) ( V m β b ) = R T \left( P+\frac{a}{V_{m}^{2}} \right)\left( {{V}_{m}}-b \right)=RT ( P + V m 2 β a β ) ( V m β β b ) = RT where Vm is the molar volume of the gas, R is the universal gas constant, T is temperature, P is pressure, a and b are the Van der Waals' constants
Find P ( V m ) P\left( {{V}_{m}} \right) P ( V m β )
P ( V m ) = R T V m β b β a V m 2 P\left( {{V}_{m}} \right)=\frac{RT}{{{V}_{m}}-b}-\frac{a}{V_{m}^{2}} P ( V m β ) = V m β β b RT β β V m 2 β a β Work done by one mole of gas during the isothermal expansion from volume V1 , to V2 at temperature T is
W = β« V 1 V 2 P ( V m ) d V m = β« V 1 V 2 ( R T V m β b β a V m 2 ) d V m W=\int\limits_{{{V}_{_{1}}}}^{{{V}_{2}}}{P\left( {{V}_{m}} \right)d{{V}_{m}}}=\int\limits_{{{V}_{_{1}}}}^{{{V}_{2}}}{\left( \frac{RT}{{{V}_{m}}-b}-\frac{a}{V_{m}^{2}} \right)d{{V}_{m}}} W = V 1 β β β« V 2 β β P ( V m β ) d V m β = V 1 β β β« V 2 β β ( V m β β b RT β β V m 2 β a β ) d V m β
W = ( R T ln β‘ ( V m β b ) + a V m ) β£ V 1 V 2 W=\left. \left( RT\ln \left( {{V}_{m}}-b \right)+\frac{a}{{{V}_{m}}} \right) \right|_{{{V}_{1}}}^{{{V}_{2}}} W = ( RT ln ( V m β β b ) + V m β a β ) β£ β£ β V 1 β V 2 β β
W = R T ( ln β‘ ( V 2 β b ) β ln β‘ ( V 1 β b ) ) + a V 2 β a V 1 W=RT\left( \ln \left( {{V}_{2}}-b \right)-\ln \left( {{V}_{1}}-b \right) \right)+\frac{a}{{{V}_{2}}}-\frac{a}{{{V}_{1}}} W = RT ( ln ( V 2 β β b ) β ln ( V 1 β β b ) ) + V 2 β a β β V 1 β a β
W = R T ln β‘ V 2 β b V 1 β b + a V 1 β V 2 V 1 V 2 W=RT\ln \frac{{{V}_{2}}-b}{{{V}_{1}}-b}+a\frac{{{V}_{1}}-{{V}_{2}}}{{{V}_{1}}{{V}_{2}}} W = RT ln V 1 β β b V 2 β β b β + a V 1 β V 2 β V 1 β β V 2 β β