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On continuous spectra of the Orr-Sommerfeld/Squire equations and entrainment of free-stream vortical disturbances in the Blasius boundary layer

机译:关于Orr-Sommerfeld / Squire方程的连续谱和Blasius边界层中自由流涡旋扰动的夹带

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Small-amplitude perturbations are governed by the linearized Navier-Stokes equations, which are, for a parallel or nearly parallel shear flow, customarily reduced to the Orr-Sommerfeld (O-S) and Squire equations. In this paper, we consider continuous spectra (CS) of the O-S and Squire operators for the Blasius boundary layer, and address the issue of whether and when continuous modes can represent free-stream vortical disturbances and their entrainment into the shear layer. We highlight two particular properties of the CS: (a) the eigenfunction of a continuous mode simultaneously consists of two components with wall-normal wavenumbers ±k_2, a phenomenon which we refer to as 'entanglement of Fourier components'; and (b) for low-frequency disturbances the presence of the boundary layer forces the streamwise velocity in the free stream to take a much larger amplitude than those of the transverse velocities. Both features appear to be non-physical, and cast some doubt about the appropriateness of using CS to characterize free-stream vortical disturbances and their entrainment into the boundary layer, a practice that has been adopted in some recent studies of bypass transition. A high-Reynolds-number asymptotic description of continuous modes and entrainment is present, and it shows that the entanglement is a result of neglecting non-parallelism, which has a leading-order effect on the entrainment. When this effect is included, entanglement disappears, and moreover the streamwise velocity is significantly amplified in the edge layer when R~(-1) ω 1, where R is the Reynolds number based on the local boundary-layer thickness.
机译:小振幅扰动由线性Navier-Stokes方程控制,对于平行或近似平行的剪切流,通常将其简化为Orr-Sommerfeld(O-S)和Squire方程。在本文中,我们考虑了Blasius边界层的O-S和Squire算子的连续谱(CS),并讨论了连续模式是否以及何时可以表示自由流涡旋扰动及其夹带到剪切层的问题。我们着重介绍了CS的两个特殊特性:(a)连续模的本征函数同时由两个具有壁法向波数±k_2的分量组成,这种现象我们称为“傅立叶分量的缠结”; (b)对于低频扰动,边界层的存在迫使自由流中的流向速度具有比横向速度大得多的幅度。这两个特征似乎都是非物理的,并且对使用CS表征自由流涡旋扰动及其夹带进入边界层的适当性提出了一些疑问,这种做法已在一些旁路过渡的最新研究中采用。存在连续模态和夹带的高雷诺数渐近描述,它表明纠缠是忽略非平行性的结果,这对夹带具有前导作用。当包括该效应时,缠结消失,并且当R〜(-1)<<ω<< 1时,在边缘层中沿流的速度显着放大,其中R是基于局部边界层厚度的雷诺数。

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