2012/08/01 by Zhengbing Chen, Alejandra Ortiz, Alejandra C. Ortiz +2 · 1 citation
Earth and Planetary Sciences · Engineering · Environmental Science · #Aeolian processes and effects #Hydrology and Sediment Transport Processes #Particle Dynamics in Fluid Flows
paper · pdf · doi:10.1029/2012wr012224
openalex publication_date 2012/08/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
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.