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Effective slip law for general viscous flows over an oscillating surface

机译:有效粘性定律,用于一般粘性流在振荡表面上的流动

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We consider the non-stationary three-dimensional viscous flow in a bounded domain, with the lateral surface containing microscopic surface irregularities. Under the assumption of a smooth flow in the domain without roughness, we prove that there is a smooth solution to a problem with the rough boundary. In the papers by J?ger and Mikelic?, the friction law was obtained as a perturbation of the Poiseuille flows. Here, the situation is more complicated. Nevertheless, after studying the corresponding boundary layers and using the results on solenoidal vector fields in domains with rough boundaries, we obtain rigorously the Navier friction condition. It is valid when the size and amplitude of the imperfections tend to zero. Furthermore, the friction matrix in the law is determined through a family of auxiliary boundary-layer type problems. Effective equations approximate velocity at order O (ε) in the H1-norm, uniformly in time, and O(ε~(3/2)) in the L ~2-norm, also uniformly in time. Approximation for the pressure is O(ε~(3/2)) in the Lloc2-norm.
机译:我们考虑边界区域中的非平稳三维粘性流,其侧面包含微观表面不规则性。假设在没有粗糙度的区域中有平滑的流动,我们证明存在粗糙边界问题的平滑解决方案。在J?ger和Mikelic?的论文中,摩擦定律是通过对Poiseuille流的扰动而获得的。在这里,情况更加复杂。但是,在研究了相应的边界层并使用具有粗糙边界的域中螺线管矢量场的结果后,我们可以精确地获得Navier摩擦条件。当瑕疵的大小和幅度趋于零时有效。此外,定律中的摩擦矩阵是通过一系列辅助边界层类型问题确定的。有效方程近似地在时间上均匀一致地表示H1范数中O(ε)的速度,并且在时间上也均匀地近似表示L〜2范数中的O(ε〜(3/2))。在Lloc2-范数中,压力的近似值为O(ε〜(3/2))。

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