Shock polar

Shock polar in the (''φ'', ''p'') plane

The minimum angle, \theta, which an oblique shock can have is the Mach angle \mu =\sin^{-1}(1/M), where M is the initial Mach number before the shock and the greatest angle corresponds to a normal shock. The range of shock angles is therefore \sin^{-1}(1/M)\leq\theta\leq\pi /2. To calculate the pressures for this range of angles, the Rankine–Hugoniot equations are solved for pressure: \frac{p}{p_{0}} = 1 + \frac{2\gamma}{\gamma +1} \left(M^{2}\sin^{2}\theta - 1\right) To calculate the possible flow deflection angles, the relationship between shock angle \theta and \varphi is used: \tan\varphi = 2\cot\theta\frac{M^{2}\sin^{2}\theta -1}{2+M^{2}(\gamma +\cos 2\theta )}. Where \gamma is the ratio of specific heats and \varphi is the flow deflection angle.

Uses of shock polars

One of the primary uses of shock polars is in the field of shock wave reflection. A shock polar is plotted for the conditions before the incident shock, and a second shock polar is plotted for the conditions behind the shock, with its origin located on the first polar, at the angle through which the incident shock wave deflects the flow. Based on the intersections between the incident shock polar and the reflected shock polar, conclusions as to which reflection patterns are possible may be drawn. Often, it is used to graphically determine whether regular shock reflection is possible, or whether Mach reflection occurs.{{cite book

References

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References

1. Busemann, A. 1929. Verdichtungsstosse in ebenen Gasstromungen. In Vortraye aus dem Gebiet der Aerodynamik, Aachen, ed. A. Gilles, L. Hopf, T. von Karman, p. 162. Berlin: Springer-Verlag