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Hydrodynamics of modulated finite-amplitude waves in dispersive media

机译:色散介质中有限振幅调制波的流体力学

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Analytic approaches are developed for integrating the nondiagonalizable Whitham equations for the generation and propagation of nonlinear modulated finite-amplitude waves in dissipationless dispersive media. Natural matching conditions for these equations are stated in a general form analogous to the Gurevich-Pitaevskii conditions for the averaged Kortewegde Vries equations. Exact relationships between the hydrodynamic quantities on different sides of a dissipationless shock wave, an analog of the shock adiabat in ordinary dissipative hydrodynamics and first proposed on the basis of physical considerations by Gurevich and Meshcherkin, ~4 are obtained. The boundaries of a self similar, dissipationless shock wave are determined analytically as a function of the density jump. Some specific examples are considered.
机译:开发了用于整合不可对角化的Whitham方程的解析方法,用于在无耗散色散介质中生成和传播非线性调制有限振幅波。这些方程式的自然匹配条件以一般形式表示,类似于平均Kortewegde Vries方程式的Gurevich-Pitaevskii条件。获得了无耗散冲击波不同侧的流体动力学量之间的精确关系,这是普通耗散流体力学中的冲击绝热体的类似物,并且首先根据Gurevich和Meshcherkin的物理考虑提出了〜4。自相似的,无耗散的冲击波的边界是根据密度跃变而解析确定的。考虑一些具体的例子。

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