Carbon dioxide is modelled by the pressure law used in the text

PHYSICS · Multi-part · Fermi University Physics · Thermal, Statistical & Complex Systems · Thermodynamic potentials and the formal structure of thermodynamics · Interacting systems, real gases and phase equilibria

Thermal Physics, Ch Thermodynamic potentials, Legendre transforms and Maxwell relations

Problem

Carbon dioxide is modelled by the pressure law used in the text, written per mole,p=nRTV−nbex−aattn2V2,p = \frac{nRT}{V - nb_{\rm ex}} - \frac{a_{\rm att}n^{2}}{V^{2}}, with nn the number of moles, R=8.314 J mol−1 K−1R = 8.314\,\mathrm{J\,mol^{-1}\,K^{-1}}, aatt=0.364 Pa m6 mol−2a_{\rm att} = 0.364\,\mathrm{Pa\,m^{6}\,mol^{-2}} and bexb_{\rm ex} a constant whose value is not needed below. A sample of n=2.00 moln = 2.00\,\mathrm{mol} is held at the fixed temperature T=300 KT = 300\,\mathrm{K} and expands quasistatically from V1=4.00 LV_1 = 4.00\,\mathrm{L} to V2=20.0 LV_2 = 20.0\,\mathrm{L} (1 L=10−3 m31\,\mathrm{L} = 10^{-3}\,\mathrm{m^{3}}). ((a)) Show, using the energy equation of a gas, that (∂U/∂V)T=aattn2/V2(\partial U/\partial V)_{T} = a_{\rm att}n^{2}/V^{2} for this gas. ((b)) Evaluate (∂U/∂V)T(\partial U/\partial V)_{T} in the initial state. ((c)) Find the change ΔU\Delta U of the internal energy in the expansion.

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