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Navier-Stokes regularization of multidimensional Euler shocks

机译:多维Euler冲击的Navier-Stokes正则化

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摘要

We establish existence and stability of multidimensional shock fronts in the vanishing viscosity limit for a general class of conservation laws with "real", or partially parabolic, viscosity including the Navier-Stokes equations of compressible gas dynamics with standard or van der Waals-type equation of state. More precisely, given a curved Lax shock solution u(0) of the corresponding inviscid equations for which (i) each of the associated planar shocks tangent to the shock front possesses a smooth viscous profile and (ii) each of these viscous profiles satisfies a uniform spectral stability condition expressed in terms of an Evans function, we construct nearby smooth viscous shock solutions u(is an element of) of the viscous equations converging to u(0) as viscosity is an element of -> 0, and establish for these sharp linearized stability estimates generalizing those of Majda in the inviscid case. Conditions (i)-(ii) hold always for shock waves of sufficiently small amplitude, but in general may fail for large amplitudes.
机译:对于具有“真实”或部分抛物线型守恒律的常规守恒律,我们在消失的粘度极限中建立了多维激波前沿的存在和稳定性,其中包括带有标准或范德华斯型方程的可压缩气体动力学的Navier-Stokes方程状态。更精确地,给定相应的无粘性方程的弯曲Lax冲击解u(0),对于该方程,(i)与冲击前沿相切的每个相关平面冲击都具有光滑的粘性轮廓,并且(ii)这些粘性轮廓中的每个满足a以Evans函数表示的均匀光谱稳定性条件,我们构造了粘性方程的附近光滑粘性激波解u(是e的元素),因为粘度是-> 0的元素,所以收敛到u(0)并为此建立尖锐的线性化稳定性估计值概括了Majda在无粘性情况下的稳定性。条件(i)-(ii)始终适用于振幅足够小的冲击波,但通常对于较大的振幅可能会失败。

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