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首页> 外文期刊>Journal of Differential Equations >Boundary layers associated with incompressible Navier-Stokes equations: The noncharacteristic boundary case
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Boundary layers associated with incompressible Navier-Stokes equations: The noncharacteristic boundary case

机译:与不可压缩的Navier-Stokes方程相关的边界层:非特征边界情况

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摘要

The goal of this article is to study the boundary layer of wall bounded flows in a channel at small viscosity when the boundaries are uniformly noncharacteristic, i.e., there is injection and/or suction everywhere at the boundary, Following earlier work on the boundary layer for linearized Navier-Stokes equations in the case where the boundaries are characteristic (no-slip at the boundary and non-permeable), we consider here the case where the boundary is permeable and thus noncharacteristic. The form of the boundary layer and convergence results are derived in two cases: linearized equation and full nonlinear equations. We prove that there exists a boundary layer at the outlet (downwind) of the form e(-Uz/e) where U is the speed of injection/suction at the boundary, : is the distance to the outlet of the channel, and 8 is the kinematic viscosity. We improve an earlier result of S. N. Alekseenko (1994, Siberian Math. J. 35, No. 2, 209 230) where the convergence in L-2 of the solutions of the Navier Stokes equations to that of the Euler equations at vanishing viscosity was established. In the two dimensional case we are able to derive the physically relevant uniform in space (L-2 norm) estimates of the boundary layer. The uniform in space estimate is derived by properly developing our previous idea of better control on the tangential derivative and the use of an anisotropic Sobolev imbedding. To the best of our knowledge this is the first rigorously proved result concerning boundary layers for the full (nonlinear) Navier Stokes equations for incompressible fluids. (C) 2002 Elsevier Science (USA). [References: 39]
机译:本文的目的是研究边界均匀一致的非粘性特性(即边界处到处都有注入和/或吸力)时,在较小粘度下通道中壁边界流的边界层。在边界为特征(边界处为非滑动且非渗透性)的情况下线性化的Navier-Stokes方程,此处我们考虑边界为渗透性且因此非特征的情况。在两种情况下得出边界层的形式和收敛结果:线性化方程和完全非线性方程。我们证明在出口处(顺风处)存在边界层,其形式为e(-Uz / e),其中U是边界处的注入/吸取速度,:是到通道出口的距离,并且8是运动粘度。我们改进了SN Alekseenko(1994,Siberian Math。J. 35,No. 2,209 230)的早期结果,其中在消失粘度下,Navier Stokes方程的解与Euler方程的解在L-2上的收敛为成立。在二维情况下,我们能够得出边界层在空间上的物理相关统一估计(L-2范数)。通过适当发展我们先前对切向导数的更好控制和使用各向异性Sobolev嵌入的思想,可以得出空间估计的统一性。据我们所知,这是关于不可压缩流体的完整(非线性)Navier Stokes方程有关边界层的第一个严格证明的结果。 (C)2002 Elsevier Science(美国)。 [参考:39]

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