FIG. 20. Cross-sectional plots ofρ, u, v, and p for the same run shown in Fig. 19 x = y.
plot, we observe sharp resolution of the primary shock waves and good behavior of the slip lines. The cross-sectional plots ofρ, u, v, and p for the same run along the line x = y provide an example of the basic structure of the solutions quantitatively. A detailed study of the algorithm to more general unstable interface problems such as the Kelvin–Helmholtz and Rayleigh–Taylor instabilities will be reported elsewhere in the future.
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