Of nitrogen, treated as a diatomic ideal gas with , is held in a cylinder closed by a…

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Thermal, Statistical & Complex Systems · Calculus of change and accumulation

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

Problem

n=0.500 moln = 0.500\ \mathrm{mol} of nitrogen, treated as a diatomic ideal gas with CV=52nRC_V = \tfrac52 nR, is held in a cylinder closed by a frictionless piston. The cylinder sits in a large bath at T=295 KT = 295\ \mathrm{K}, and the gas is expanded quasistatically and isothermally from 3.00 L3.00\ \mathrm{L} to 9.00 L9.00\ \mathrm{L}. Write NkB=nRNk_B = nR. Chapter 3's convention ΔU=Q+W\Delta U = Q + W is used, with WW the work done on the gas. ((a)) Show that δQ=52nR dT+nRTV dV\delta Q = \tfrac52 nR\,\mathrm{d}T + \dfrac{nRT}{V}\,\mathrm{d}V, the heat delivered to this gas in a quasistatic step, is not an exact differential in TT and VV, and say what that means for the phrase "the heat content of the gas". ((b)) Find ΔF\Delta F for the gas in this expansion. ((c)) Find the work the gas delivers, and state why it reaches the bound set by ΔF\Delta F. ((d)) Find the entropy change of the bath.

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