Vortex development behind a finite porous obstruction in a channel
By Lijun Zong, H. Nepf. Journal of Fluid Mechanics, 2011
256 citations recorded by the source corpus.
Abstract This experimental study describes the turbulent wake behind a two-dimensional porous obstruction, consisting of a circular array of cylinders. The cylinders extend from the channel bed through the water surface, mimicking a patch of emergent vegetation. Three patch diameters ($D$) and seven solid volume fractions ($\Phi $) are tested. Because flow can pass through the patch, directly downstream there is a region of steady, non-zero, streamwise velocity, ${U}_{1} $, called the steady wake. For the patch diameters and solid volume fractions considered here, ${U}_{1} $ is a function of $\Phi $ only. The length of the steady wake (${L}_{1} $) increases as $\Phi $ decreases and can be predicted from the growth of a plane shear layer. The formation of the von-Kármán vortex street is delayed until the end of the steady wake. There are two regions of elevated transverse velocity fluctuation (${v}_{\mathit{rms}} $): directly behind the patch, associated with the wake turbulence of individual cylinders; and at the distance ${L}_{1} $ from the patch, associated with the formation of large-scale wake oscillation. Velocity along the centreline of the wake starts to increase only after the patch-scale vortex street is formed, and it approaches the free-stream velocity over a distance ${L}_{2} $. The dimensionless length of the entire wake, $({L}_{1} + {L}_{2} )/ D$, increases with patch porosity.
Subfields: Computational Mechanics, Earth-Surface Processes, Ecology
View Paper: https://www.semanticscholar.org/paper/2e7bb813999a4c27fda8cc679b8b99a9d892d278
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In Computational Mechanics
- Fotis Sotiropoulos
- Roger E. A. Arndt
- Leonardo P. Chamorro
- Xiaolei Yang
- Fernando Port'e-Agel
- Seokkoo Kang
In Earth-Surface Processes
Citations in the corpus
- On the interaction between a turbulent open channel flow and an axial-flow turbine (2013, background): “Zong & Nepf (2012) have reported in detail a similar phenomenon (stable region followed by a meandering motion) for the case of a finite porous obstruction placed in an open channel flow.”