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Concerning the W ~(k,p) -Inviscid Limit for 3-D Flows Under a Slip Boundary Condition

机译:关于滑移边界条件下3-D流的W〜(k,p)-无粘极限

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We consider the 3-D evolutionary Navier-Stokes equations with a Navier slip-type boundary condition, see (1.2), and study the problem of the strong convergence of the solutions, as the viscosity goes to zero, to the solution of the Euler equations under the zero-flux boundary condition. We prove here, in the flat boundary case, convergence in Sobolev spaces W (k, p) (Omega), for arbitrarily large k and p (for previous results see Xiao and Xin in Comm Pure Appl Math 60:1027-1055, 2007 and Beiro da Veiga and Crispo in J Math Fluid Mech, 2009, doi:10.1007/s00021-009-0295-4). However this problem is still open for non-flat, arbitrarily smooth, boundaries. The main obstacle consists in some boundary integrals, which vanish on flat portions of the boundary. However, if we drop the convective terms (Stokes problem), the inviscid, strong limit result holds, as shown below. The cause of this different behavior is quite subtle. As a by-product, we set up a very elementary approach to the regularity theory, in L (p) -spaces, for solutions to the Navier-Stokes equations under slip type boundary conditions.
机译:我们考虑具有Navier滑移型边界条件的3-D演化Navier-Stokes方程,请参阅(1.2),并研究随着粘度变为零而向Euler解的溶液的强收敛问题。零通量边界条件下的方程。我们在这里证明,在平坦边界情况下,对于任意大的k和p,在Sobolev空间W(k,p)(Omega)中收敛(有关先前的结果,请参见com Pure Appl Math 60:1027-1055,2007中的Xiao和Xin)和Beiro da Veiga和Crispo着,《 J Math Fluid Mech》,2009年,doi:10.1007 / s00021-009-0295-4)。但是,对于非平坦,任意平滑的边界,这个问题仍然存在。主要障碍在于一些边界积分,这些积分在边界的平坦部分上消失。但是,如果我们删除对流项(斯托克斯问题),则无粘性的强极限结果成立,如下所示。这种不同行为的原因非常微妙。作为副产品,我们为L(p)空间中的正则性理论建立了非常基本的方法,用于解决滑动类型边界条件下的Navier-Stokes方程。

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