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首页> 外文期刊>Journal of Fluid Mechanics >On the influence of Sommerfeld's radiation boundary condition on the propagation direction of oblique modes in streamwise corner flow
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On the influence of Sommerfeld's radiation boundary condition on the propagation direction of oblique modes in streamwise corner flow

机译:Sommerfeld辐射边界条件对斜向流在角流中传播方向的影响

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Linear stability of a laminar boundary-layer flow in a streamwise corner can only be treated with an ansatz that considers two-dimensional eigenfunctions with inhomogeneous boundary conditions in cross-flow directions. It is common practice to use Sommerfeld's radiation condition with a certain wavenumber beta at the lateral domains of the integration domain which are at the same time the far-field domains for each wall. So far, this radiation condition has been exclusively used in a 'symmetrical' way, i.e. with the same beta on either far-field boundary plane. This has led to wave patterns that either enter or leave the corner region from the lateral sides for beta < 0 or beta > 0 respectively. Here, an 'asymmetric' use of Sommerfeld's radiation condition is suggested, i.e. beta < 0 on one far side of the corner and beta > 0 on the other. With this modification, waves enter the corner area from one side and leave it through the other, i.e. they travel obliquely through the corner. In contrast to before, their amplification rate is always symmetric with respect to beta = 0 and there is no amplification-rate increase or decrease due to information that either continuously enters the corner from both sides or continuously leaves it through the far sides. The present analysis also shows that the inviscid corner modes are unaffected by the parameters of the far-field radiation boundary conditions. Nevertheless, superposition of two oppositely running single waves obtained by the modified application of the radiation condition leads to a similar wave pattern to that in the case with beta < 0 on both sides; however, with a slightly smaller amplification rate and a strictly streamwise propagation direction.
机译:流向角部中层流边界层流的线性稳定性只能使用考虑了二维本征函数且边界条件在横向流方向上不均匀的ansatz来处理。通常的做法是使用Sommerfeld辐射条件,并在积分域的横向域使用一定的波数β,这些边域同时是每面墙的远场域。到目前为止,仅以“对称”方式使用此辐射条件,即在任一远场边界平面上具有相同的beta。这导致了波型从侧面分别进入或离开角区域的beta <0或beta> 0。在这里,建议使用Sommerfeld辐射条件的“非对称”使用,即在拐角的一个远侧的beta <0,在另一侧的beta> 0。通过这种修改,波浪从一侧进入拐角区域,并从另一侧离开,即它们倾斜地穿过拐角。与以前相反,它们的放大率始终相对于beta = 0是对称的,并且由于信息从两侧连续进入拐角或从远端连续离开拐角而导致的放大率没有增加或减少。目前的分析还表明,无角转角模式不受远场辐射边界条件参数的影响。然而,通过修改辐射条件的应用获得的两个反向运行的单波的叠加导致了与两侧β<0的情况类似的波型;但是,放大率稍小,并且沿流方向严格地传播。

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