三维交错波壁湍流中的二次流和向流涡

IF 2.8 Q2 MECHANICS Flow (Cambridge, England) Pub Date : 2023-07-04 DOI:10.1017/flo.2023.13
Enwei Zhang, Zhan Wang, Wangxia Wu, Xiaoliang Wang, Qing-quan Liu
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引用次数: 0

摘要

摘要本文将自然形成的沙丘(河床)简化为大型三维交错波浪墙,通过大涡模拟研究伴随的二次流和流向涡的特征。涡流强度和平均速度之间的比较表明,二次流在哪里引起上洗或下洗运动。此外,我们提出了一种伪凸壁机制来解释二次流的方向性。离心失稳准则随后被用来揭示流向涡流的产生。基于这些分析结果,我们发现在特征纵向、垂直和水平截面上的分离点和再附着点都会产生顺流涡流,这与湍流剪切层的曲率效应有关。此外,以离心与粘性效应之比为特征的最大Görtler数表明,对于展向与流向波长之比固定的情况,随着振幅的增加,发生在纵向-垂直截面上的最强离心不稳定性逐渐占主导地位。对于具有不同展向波长的情况,也可以发现类似的趋势。还发现,当展向与流向波长之比等于1时,流向涡流更容易通过分离点和再附着点附近波峰周围的横向流动产生。
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Secondary flow and streamwise vortices in three-dimensional staggered wavy-wall turbulence
Abstract The present paper simplifies the naturally formed dunes (riverbeds) as large-scale three-dimensional staggered wavy walls to investigate the features of the accompanying secondary flows and streamwise vortices via large-eddy simulation. A comparison between the swirling strength and the mean velocities suggests where a secondary flow induces upwash or downwash motions. Moreover, we propose a pseudo-convex wall mechanism to interpret the directionality of the secondary flow. The centrifugal instability criterion is then used to reveal the generation of the streamwise vortices. Based on these analytical results, we found that the streamwise vortices are generated in the separation and reattachment points on both characteristic longitudinal–vertical and horizontal cross-sections, which is related to the curvature effect of the turbulent shear layer. Furthermore, the maximum Görtler number characterized by the ratio of centrifugal to viscous effects suggests that, for fixed ratio of spanwise- to streamwise-wavelength cases, the strongest centrifugal instability occurring on the longitudinal–vertical cross-section gradually dominates with the increases in amplitude. A similar trend for the cases with varied spanwise wavelength can also be found. It is also found that the streamwise vortices are generated more readily via transverse flow around the crest near the separation and reattachment points when the ratio of spanwise- to streamwise-wavelength equals 1.
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2.40
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