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A kinetic model of the Boltzmann equation for non-vibrating polyatomic gases

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Figure

Figure 1with DSMC results. As expected, our kinetic model resolves the problem of earlyrising of the temperatures, and produces results in good agreement with the DSMC compares the normal shock profiles obtained by the two kinetic modelsdata.
FIGURELand the experimental data of Robben & Talbot ( 2. Comparisons of normal shock wave profiles in nitrogen from our kinetic model1966): (a) Ma = 7; (b) Ma = 12.9
TABLE 1. Mass (M ) and translational heat (Qt) flow rates in Poiseuille flow of a hard-sphere diatomic gas between parallel plates
FIGURE(lines) to the experimental data (dots) of Gu & Ubachs (2336 8. (Colour online) Spontaneous RBS spectra for nitrogen, comparing our model2013)
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