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Table 1 Variation of the density ratio \(\beta \left( =\dfrac{\rho _{a}}{\rho _{n}}\right)\) across the shock front and the position of the piston surface \(\xi _{p}\) for different values of \(M_{A}^{-2}\), \(\gamma\) and \(\dfrac{\sigma }{i}\)

From: Flow behind an exponential shock wave in a rotational axisymmetric perfect gas with magnetic field and variable density

\(M_{A}^{-2}\)

\(\gamma\)

\(\beta\)

Position of the piston surface \(\xi _{p}\)

Isothermal flow

Adiabatic flow

\(\dfrac{\sigma }{i} = 1\)

\(\dfrac{\sigma }{i} = 1.5\)

\(\dfrac{\sigma }{i} = 1\)

\(\dfrac{\sigma }{i} = 1.5\)

0

\(\dfrac{4}{3}\)

0.142857

0.899886

0.834074

0.956562

0.951338

\(\dfrac{5}{3}\)

0.25000

0.822819

0.690086

0.917366

0.908795

0.01

\(\dfrac{4}{3}\)

0.165804

0.892594

0.835098

0.934578

0.925728

\(\dfrac{5}{3}\)

0.261039

0.823930

0.705373

0.904250

0.892942

0.1

\(\dfrac{4}{3}\)

0.296396

0.840903

0.800793

0.856906

0.836709

\(\dfrac{5}{3}\)

0.34838

0.808796

0.744513

0.842153

0.820695