Fig. 4

Propagation and amplification of a 100 kms-1 or M = 0.01 perturbation in the planar density gradient. In blue the velocity from the numerical simulation, compared to the amplification of Eq. (2) in the absence of dissipation. They separate when the shocks kinetic energy is dissipated. This is stressed by the temperature at three subsequent times plotted in black.
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