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Local boundary-layer receptivity to a convected free-stream disturbance

机译:对流自由流扰动的局部边界层接受性

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摘要

An investigation of the local receptivity of a Blasius boundary layer to a harmonic vortical disturbance is presented as a step towards understanding boundary-layer receptivity to free-stream turbulence. Although there has been solid experimental verification of the linear theory describing acoustic receptivity of boundary layers, this was the first experimental verification of the mechanism behind local receptivity to a convected disturbance. The harmonic wake from a vibrating ribbon positioned upstream of a flat plate provided the free-stream disturbance. Two-dimensional roughness elements on the surface of the plate acted as a local receptivity site. Hot-wire measurements in the boundary layer downstream of the roughness confirmed the generation of Tollmien-Schlichting (TS) instability waves by an outer-layer interaction between the long-wavelength convected disturbance and the short-scale mean-flow distortion due to the roughness. The characteristics of the instability waves were carefully measured to ensure that their behaviour was correctly modelled by linear stability theory. This theory was then used to determine the immeasurably small initial wave amplitudes resulting from the receptivity process, from wave amplitudes measured downstream. Tests were performed to determine the range of validity of the linear assumptions made in current receptivity theories. Experimental data obtained in the linear regime were then compared to theoretical results of other authors by expressing the experimental data in the form of an efficiency function which is independent of the free-stream amplitude, roughness height and roughness geometry. Reasonable agreement between the experimental and theoretical efficiency functions was obtained over a range of frequencies and Reynolds numbers.
机译:提出了对Blasius边界层对谐波涡旋扰动的局部接受度的研究,作为迈向了解边界层对自由流湍流的接受度的一步。尽管已经对描述边界层的声接收性的线性理论进行了可靠的实验验证,但这是对对流干扰的局部接收性背后机理的首次实验验证。来自位于平板上游的振动带的谐波唤醒提供了自由流干扰。平板表面上的二维粗糙度元素充当局部接受位置。在粗糙度下游的边界层中进行的热线测量证实了长波对流扰动与粗糙度引起的短尺度平均流畸变之间的外层相互作用,从而产生了托尔米-施利希特(TS)不稳定性波。仔细测量了不稳定波的特性,以确保通过线性稳定性理论正确地模拟了它们的行为。然后,使用该理论来确定从接收过程中得出的,由下游测得的波幅而产生的很小的初始波幅。进行测试以确定在当前接受理论中所做的线性假设的有效性范围。然后,以效率函数的形式表示实验数据,将线性状态下获得的实验数据与其他作者的理论结果进行比较,该效率函数独立于自由流振幅,粗糙度高度和粗糙度几何形状。在一定频率和雷诺数范围内,获得了实验效率函数和理论效率函数之间的合理一致性。

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