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首页> 外文期刊>Journal of Fluid Mechanics >On scaling pipe flows with sinusoidal transversely corrugated walls: analysis of data from the laminar to the low-Reynolds-number turbulent regime
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On scaling pipe flows with sinusoidal transversely corrugated walls: analysis of data from the laminar to the low-Reynolds-number turbulent regime

机译:在具有正弦形横向波纹壁的缩放管流上:对层流到低雷诺数湍流状态的数据的分析

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Direct numerical simulation was used to study laminar and turbulent flows in circular pipes with smoothly corrugated walls. The corrugation wavelength was kept constant at 0.419D, where D is the mean diameter of the wavy-wall pipe and the corrugation height was varied from zero to 0.08D. Flow rates were varied in steps between low values that generate laminar flow and higher values where the flow is in the post-transitional turbulent regime. Simulations in the turbulent regime were also carried out at a constant Reynolds number, Re-tau=314, for all corrugation heights. It was found that even in the laminar regime, larger-amplitude corrugations produce flow separation. This leads to the proportion of pressure drop attributable to pressure drag being approximately 50 %, and rising to approximately 85 % in transitional rough-wall flow. The near-wall structure of turbulent flow is seen to be heavily influenced by the effects of flow separation and reattachment. Farther from the wall, the statistical profiles examined exhibit behaviours characteristic of smooth-wall flows or distributed roughness rough-wall flows. These observations support Townsend's wall-similarity hypothesis. The organized nature of the present roughness allows the mean pressure drop to be written as a function of the corrugation height. When this is exploited in an analysis of the mean dynamical equation, the scaling problem is explicitly revealed to result from the combined influences of roughness and Reynolds number. The present results support the recent analysis and observations of Mehdi et al. (J. Fluid Mech., vol. 731, 2013, pp. 682712), indicating that the length scale given by the distance from the wall at which the mean viscous force loses leading order is important to describing these combined influences, as well as providing a dynamically self-consistent connection to the scaling structure of smooth-wall pipe flow.
机译:直接数值模拟用于研究具有光滑波纹壁的圆形管道中的层流和湍流。波纹波长保持恒定在0.419D,其中D是波浪形壁管的平均直径,波纹高度从零变化到0.08D。流速在产生层流的低值和在过渡后湍流状态下的较高值之间逐步变化。对于所有波纹高度,还以恒定的雷诺数Re-tau = 314进行了湍流状态下的模拟。已经发现,即使在层流状态下,较大幅度的波纹也会产生流动分离。这导致可归因于压力阻力的压降比例约为50%,在过渡粗糙壁流中上升至约85%。湍流的近壁结构被认为受流分离和重新附着的影响很大。在离墙较远的地方,所检验的统计轮廓显示了光滑壁流或分布粗糙粗糙壁流的行为特征。这些观察结果支持了汤森德的壁相似性假设。当前粗糙度的有组织的特性允许将平均压降写为波纹高度的函数。当在平均动力学方程分析中利用这一点时,显式揭示了定标问题是由粗糙度和雷诺数的综合影响导致的。目前的结果支持了Mehdi等人的最新分析和观察。 (J. Fluid Mech。,第731卷,2013年,第682712页),表明长度尺度是由与平均粘性力失去前导顺序的壁的距离给出的,对于描述这些综合影响以及提供与平滑壁管道流量缩放结构的动态自洽连接。

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