The shock wave instability induced when interacting with a small waviness on an interface with plasma was investigated analytically and numerically. The perturbation to the shock was phenomenologically treated assuming… Click to show full abstract
The shock wave instability induced when interacting with a small waviness on an interface with plasma was investigated analytically and numerically. The perturbation to the shock was phenomenologically treated assuming this as the consequence of the shock refraction. The instability develops in the form of wave-like stretchings into lower density plasma followed with the loss of stability in the flow behind it, and eventually evolving into an intense vortex structure. The instability mode is aperiodical and unconditional, and either a transition to another stable state or continuous development as a secondary flow is possible. Among other interesting features are: a similarity law in the spatial and temporal evolution of the perturbations with respect to the interface curvature; the instability locus independence of the gas density distribution, thus identifying the interface conditions as the sole triggering factor; the role of the density gradient in the instability evolution discriminating between qualitatively different outcomes; and the possibility of decay via nonviscous damping mechanisms. The phenomenological connection between the shockâs and the interface stability is discussed.
               
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