Q1(c). Internal pressure (∂ U/∂ V)_T of a van der Waals gas
van der Waals' equation states that (P+a V²)( V-b)=RT (a and b are constants).
Find ((∂ u)/(∂ v))_T for van der Waals' gas.
Answer in brief
((∂ Uₘ)/(∂ Vₘ))_T=a V²: positive, and set by the attraction constant a alone.
Key points
- dU=T dS-P dV. Divide by dV at constant T: ((∂ U)/(∂ V))_T=T((∂ S)/(∂ V))_T-P
- ((∂ S)/(∂ V))_T=((∂ P)/(∂ T))_V. Hence the thermodynamic equation of state ((∂ U)/(∂ V))_T=T((∂ P)/(∂ T))_V-P
- P=(RT)/( V-b)-a V², so ((∂ P)/(∂ T))_V=(R)/( V-b)
- T·(R)/( V-b)-((RT)/( V-b)-a V²), ((∂ Uₘ)/(∂ Vₘ))_T=a V²
The full model answer
Written out in full, as it should go in the answer booklet. The solution page with its diagrams follows it.
The printed u and v are read as the molar energy and molar volume, Uₘ and V.
- Fundamental equation: dU=T dS-P dV. Divide by dV at constant T: ((∂ U)/(∂ V))_T=T((∂ S)/(∂ V))_T-P
- Maxwell relation (from dA=-S dT-P dV): ((∂ S)/(∂ V))_T=((∂ P)/(∂ T))_V. Hence the thermodynamic equation of state ((∂ U)/(∂ V))_T=T((∂ P)/(∂ T))_V-P
- van der Waals gas: P=(RT)/( V-b)-a V², so ((∂ P)/(∂ T))_V=(R)/( V-b)
- Substitute: T·(R)/( V-b)-((RT)/( V-b)-a V²), ((∂ Uₘ)/(∂ Vₘ))_T=a V²
- Meaning: this is the internal pressure. Pulling molecules apart against their attraction raises U; b (repulsion) drops out. For an ideal gas a=0 and U does not depend on volume (Joule).
- Integrated form: Uₘ=Uₘ^(ideal)(T)-(a)/( V), so an isothermal expansion from V₁ to V₂ needs Δ Uₘ=a((1)/( V₁)-(1)/( V₂))>0.
Application. in a Joule expansion into a vacuum (q=w=0, Δ U=0) the energy needed comes from the kinetic energy of the molecules, so a van der Waals gas cools: Δ T=-aC_(V,m)((1)/( V₁)-(1)/( V₂)). The related Joule–Thomson throttling is the basis of gas liquefaction.
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