The wake structure behind a porous obstruction and its implications for deposition near a finite patch of emergent vegetation

唤醒 湍流 阻力 卡尔曼漩涡街 涡流 物理 湍流动能 机械 圆柱 流量(数学) 阻力系数 尾流紊流 几何学 长度刻度 粒子图像测速 雷诺数 数学
作者
Zhengbing Chen,Alejandra C. Ortiz,Lijun Zong,Heidi Nepf
出处
期刊:Water Resources Research [Wiley]
卷期号:48 (9) 被引量:170
标识
DOI:10.1029/2012wr012224
摘要

This experimental study describes the mean and turbulent flow structure in the wake of a circular array of cylinders, which is a model for a patch of emergent vegetation. The patch diameter, D , and patch density, a (frontal area per volume), are varied. The flow structure is linked to a nondimensional flow blockage parameter, C D aD , which is the ratio of the patch diameter and a drag length scale ( C D a ) −1 . C D is the cylinder drag coefficient. The velocity exiting the patch, U e , is reduced relative to the upstream velocity, U ∞ , and U e / U ∞ decreases as flow blockage ( C D aD ) increases. A predictive model is developed for U e / U ∞ . The wake behind the patch contains two peaks in turbulence intensity. The first peak occurs directly behind the patch and is related to turbulence production within the patch at the scale of individual cylinders. The second peak in turbulence intensity occurs at distance L w downstream from the patch and is related to the wake‐scale vortices of the von Karman vortex street. The presence of the flow U e in the wake delays the formation of the von Karman vortex street until distance L 1 (< L w ) behind the patch. Both L 1 and L w increase as U e increases and thus as the flow blockage ( C D aD) decreases. L 1 sets the distance behind the patch within which fine‐particle deposition can occur. Beyond L w , turbulence associated with the wake‐scale vortices inhibits deposition.

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