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Nonlinear stability of strong rarefaction waves for compressible Navier-Stokes equations

机译:可压缩的Navier-Stokes方程的强稀疏波的非线性稳定性

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摘要

This paper is concerned with the time-asymptotic behavior toward strong rarefaction waves of solutions to one-dimensional compressible Navier-Stokes equations. Assume that the corresponding Riemann problem to the compressible Euler equations can be solved by rarefaction waves (V-R, U-R, S-R)(t, x). If the initial data (v(0), u(0), s(0))(x) to the nonisentropic compressible Navier-Stokes equations is a small perturbation of an approximate rarefaction wave constructed as in [ S. Kawashima, A. Matsumura, and K. Nishihara, Proc. Japan Acad. Ser. A, 62 (1986), pp. 249-252], then we show that, for the general gas, the Cauchy problem admits a unique global smooth solution (v, u, s)(t, x) which tends to (V-R, U-R, S-R)(t, x) as t tends to infinity. A global stability result can also be established for the nonisentropic ideal polytropic gas, provided that the adiabatic exponent gamma is close to 1. Furthermore, we show that for the isentropic compressible Navier-Stokes equations, the corresponding global stability result holds, provided that the resulting compressible Euler equations are strictly hyperbolic and both characteristical fields are genuinely nonlinear. Here, global stability means that the initial perturbation can be large. Since we do not require the strength of the rarefaction waves to be small, these results give the nonlinear stability of strong rarefaction waves for the one-dimensional compressible Navier-Stokes equations.
机译:本文关注一维可压缩Navier-Stokes方程解对强稀疏波的时间渐近行为。假设可以通过稀疏波(V-R,U-R,S-R)(t,x)来解决可压缩的Euler方程所对应的黎曼问题。如果非等熵可压缩Navier-Stokes方程的初始数据(v(0),u(0),s(0))(x)是对在[S. Kawashima,A.松村(Matsumura)和西原K.日本学院老师A,62(1986),pp。249-252],那么我们证明,对于一般气体,柯西问题接受了唯一的全局光滑解(v,u,s)(t,x),该解趋于(VR ,UR,SR)(t,x),因为t趋于无穷大。如果绝热指数γ接近于1,则也可以为非等熵理想多变气体建立整体稳定性结果。此外,我们证明对于等熵可压缩Navier-Stokes方程,只要满足以下条件,相应的整体稳定性结果成立。由此产生的可压缩Euler方程严格是双曲的,并且两个特征场都是真正的非线性。在这里,全局稳定性意味着初始扰动可能很大。由于我们不要求稀疏波的强度较小,因此这些结果为一维可压缩Navier-Stokes方程提供了强稀疏波的非线性稳定性。

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