A figure plots for dilute carbon monoxide gas (CO

PHYSICS · Multi-part · Fermi University Physics · Thermal, Statistical & Complex Systems · Statistical mechanics of ideal classical systems · Statistical mechanics of ideal classical systems

Thermal Physics, Ch The classical ideal gas from the partition function

Problem

A figure plots CV/NkBC_V/Nk_B for dilute carbon monoxide gas (CO, treated as an ideal gas at every temperature shown, an idealisation at the lowest ones) against log⁡10(T/K)\log_{10}(T/\mathrm{K}) from 1 K1\,\mathrm{K} to 4000 K4000\,\mathrm{K}. The plotted curve is described completely by:flat at 1.501.50 for T≤1.5 KT \le 1.5\,\mathrm{K};rising steeply between about 2 K2\,\mathrm{K} and 10 K10\,\mathrm{K};flat at 2.502.50 from about 15 K15\,\mathrm{K} to about 600 K600\,\mathrm{K};rising again above about 800 K800\,\mathrm{K}, passing through 3.413.41 at 3000 K3000\,\mathrm{K}. For CO the characteristic temperatures are θrot=2.8 K\theta_{\rm rot} = 2.8\,\mathrm{K} and θvib=3120 K\theta_{\rm vib} = 3120\,\mathrm{K}. Take R=8.314 J K−1 mol−1R = 8.314\,\mathrm{J\,K^{-1}\,mol^{-1}}. Say which internal motion switches on at each of the two steps, quoting the characteristic temperature that places it there, and then: ((a)) read CV/NkBC_V/Nk_B off the plot at 1.2 K1.2\,\mathrm{K}, at 200 K200\,\mathrm{K} and at 3000 K3000\,\mathrm{K}; ((b)) convert the 200 K200\,\mathrm{K} reading into a molar heat capacity CVC_V; ((c)) state the vibrational contribution to CVC_V per molecule at 3000 K3000\,\mathrm{K}, in units of kBk_B.

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