Blundell Thermal Physics · Problem 32.2

Shock waves

Physics — Statistical Mechanics · rankine-hugoniot-temperature-ratio

Problem

Use eqn 32.24 to show that T2T1=[2γM12−(γ−1)][2+(γ−1)M12](γ+1)2M12,(32.29)\frac{T_2}{T_1} = \frac{[2\gamma M_1^2 - (\gamma - 1)][2 + (\gamma - 1)M_1^2]}{(\gamma + 1)^2 M_1^2}, \tag{32.29} and hence for M1≫1M_1 \gg 1 we have that T2T1→2γ(γ−1)M12(γ+1)2.(32.30)\frac{T_2}{T_1} \to \frac{2\gamma(\gamma - 1)M_1^2}{(\gamma + 1)^2}. \tag{32.30}

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