Van der Waals equation of state for one mole of a real gas is
( P + a V m 2 ) ( V m − b ) = R T \left( P+\frac{a}{V_{m}^{2}} \right)\left( {{V}_{m}}-b \right)=RT ( P + V m 2 a ) ( V m − 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 )
P ( V m ) = R T V m − b − a V m 2 P\left( {{V}_{m}} \right)=\frac{RT}{{{V}_{m}}-b}-\frac{a}{V_{m}^{2}} P ( V m ) = V m − b RT − V m 2 a Work done by one mole of gas during the isothermal expansion from volume V1 , to V2 at temperature T is
W = ∫ V 1 V 2 P ( V m ) d V m = ∫ V 1 V 2 ( R T V m − b − 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 ∫ V 2 P ( V m ) d V m = V 1 ∫ V 2 ( V m − b RT − V m 2 a ) d V m
W = ( R T ln ( V m − b ) + a V m ) ∣ 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 − b ) + V m a ) ∣ ∣ V 1 V 2
W = R T ( ln ( V 2 − b ) − ln ( V 1 − b ) ) + a V 2 − 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 − b ) − ln ( V 1 − b ) ) + V 2 a − V 1 a
W = R T ln V 2 − b V 1 − b + a V 1 − 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 − b V 2 − b + a V 1 V 2 V 1 − V 2
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