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Existence and stability of noncharacteristic boundary layers for the compressible navier-stokes and viscous MHD equations

机译:可压缩航鼻和粘性MHD方程非特征边界层的存在和稳定性

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For a general class of hyperbolic-parabolic systems including the compressible Navier-Stokes and compressible MHD equations, we prove existence and stability of noncharacteristic viscous boundary layers for a variety of boundary conditions including classical Navier-Stokes boundary conditions. Our first main result, using the abstract framework established by the authors in the companion work (Gues et al. in J Differ Equ, 244, 309-387 (2008)), is to show that existence and stability of arbitrary amplitude exact boundary layer solutions follow from a uniform spectral stability condition on layer profiles that is expressible in terms of an Evans function (uniform Evans stability). Whenever this condition holds we give a rigorous description of the small viscosity limit as the solution of a hyperbolic problem with "residual" boundary conditions. Our second is to show that uniform Evans stability for small-amplitude layers is equivalent to Evans stability of the limiting constant layer, which in turn can be checked by a linear-algebraic computation. Finally, for a class of symmetric-dissipative systems including the physical examples mentioned above, we carry out energy estimates showing that constant (and thus small-amplitude) layers always satisfy uniform Evans stability. This yields existence of small-amplitude multi-dimensional boundary layers for the compressible Navier-Stokes and MHD equations. For both equations these appear to be the first such results in the compressible case.
机译:对于包括可压缩的Navier-Stokes和可压缩的MHD方程在内的一类一般的双曲抛物线系统,我们证明了包括经典Navier-Stokes边界条件在内的各种边界条件的非特征粘性边界层的存在和稳定性。我们使用作者在同伴工作中建立的抽象框架(Gues等人在J Differ Equ,244,309-387(2008)中建立的抽象框架)的第一个主要结果是,表明任意幅度精确边界层的存在和稳定性解决方案来自层轮廓上的均匀光谱稳定性条件,该条件可以用伊文思函数表示(均匀伊文思稳定性)。每当这种情况成立时,我们都会严格描述小粘度极限,以解决带有“剩余”边界条件的双曲线问题。我们的第二个结果表明,小振幅层的均匀Evans稳定性等于极限常数层的Evans稳定性,这又可以通过线性代数计算来检查。最后,对于包括上述物理示例的一类对称耗散系统,我们进行了能量估计,表明恒定(因此,小振幅)层始终满足一致的Evans稳定性。这为可压缩的Navier-Stokes和MHD方程提供了小振幅的多维边界层。对于这两个方程,在可压缩情况下,这似乎是第一个这样的结果。

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