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Flow noise induced by small gaps in low-Mach-number turbulent boundary layers

机译:低马赫数湍流边界层中的小间隙引起的流动噪声

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The flow-noise induced by small gaps underneath low-Mach-number turbulent boundary layers at Reθ = 4755 is studied using large-eddy simulation and Lighthill's theory. The gap leading-edge height is 13% of the boundary-layer thickness, and the gap width and trailing-edge height are varied to investigate their effects on surface-pressure fluctuations and sound generation. The maximum surface pressure fluctuations, which increase with gap width and trailing-edge height, occur at the trailing edge or near the reattachment point if there is separation from the trailing edge. The downstream recovery towards an equilibrium boundary layer is significantly faster for gap flows compared to step flows, and the recovery distance scales with the reattachment length for gaps with trailing-edge separation. The acoustic field is dominated by the forward-facing step in the gap and resembles forward-step sound for wide gaps and/or asymmetric gaps with trailing edge higher than leading edge. In these cases, the dominant acoustic source mechanisms are the impingement of the separated shear layer from the leading edge onto the trailing edge and the unsteady separation from the trailing edge, coupled with edge diffraction. For narrow and symmetric gaps, the destructive interference of sound from the leading and trailing edges causes a significant decline in low-frequency sound and thereby creates a broad spectral peak in the mid-frequency range. The effects of gap acoustic non-compactness and free-stream convection are investigated by comparing solutions based on a compact gap Green's function with those from a boundary-element calculation. They are found to be negligible at the typical hydroacoustc Mach number of 0.01, but become significant at Mach numbers as low as 0.1 and moderately high frequencies.
机译:利用大涡模拟和Lighthill理论研究了低马赫数湍流边界层在Reθ= 4755处由小间隙引起的流动噪声。间隙的前缘高度为边界层厚度的13%,并且改变间隙的宽度和后缘的高度以研究它们对表面压力波动和声音产生的影响。如果与后边缘分离,则最大表面压力波动会随间隙宽度和后边缘高度而增加,出现在后边缘或重新连接点附近。与阶跃流相比,间隙流向平衡边界层的下游恢复要快得多,并且恢复距离随具有后缘分离的间隙的重新附着长度而定。声场由间隙中的前向台阶主导,并且类似于宽间隙和/或不对称间隙且后缘高于前缘的前向声音。在这些情况下,主要的声源机制是将分离的剪切层从前边缘撞击到后边缘,以及从后边缘不稳定地分离,再加上边缘衍射。对于狭窄且对称的间隙,来自前缘和后缘的声音的破坏性干扰会导致低频声音显着下降,从而在中频范围内产生一个宽频谱峰。通过比较基于紧凑间隙格林函数的解与边界元素计算的解,研究了间隙声学非紧凑性和自由流对流的影响。发现它们在典型的水声马赫数为0.01时可以忽略不计,但是在低至0.1的马赫数和中等频率的情况下变得很重要。

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