Shock polar

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

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.^[2][3]

• Chapman, C.J. (2000). High Speed Flow. CUP. ISBN 978-0-521-66169-0.
• Anderson, John D. Jr. (January 2001) [1984]. Fundamentals of Aerodynamics (3rd ed.). McGraw-Hill Science/Engineering/Math. ISBN 978-0-07-237335-6.