Thermally driven exchange flow between open water and an aquatic canopy

Differential solar heating can result from shading by rooted emergent aquatic plants, producing a temperature difference between vegetated and unvegetated regions of a surface water body. This temperature difference will promote an exchange flow between the vegetation and open water. Drag associated...

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Bibliographic Details
Main Authors: Nepf, Heidi (Contributor), Zhang, Xueyan (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Civil and Environmental Engineering (Contributor)
Format: Article
Language:English
Published: Cambridge University Press, 2010-12-09T16:27:46Z.
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Online Access:Get fulltext
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100 1 0 |a Nepf, Heidi  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Civil and Environmental Engineering  |e contributor 
100 1 0 |a Nepf, Heidi  |e contributor 
100 1 0 |a Nepf, Heidi  |e contributor 
100 1 0 |a Zhang, Xueyan  |e contributor 
700 1 0 |a Zhang, Xueyan  |e author 
245 0 0 |a Thermally driven exchange flow between open water and an aquatic canopy 
260 |b Cambridge University Press,   |c 2010-12-09T16:27:46Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/60254 
520 |a Differential solar heating can result from shading by rooted emergent aquatic plants, producing a temperature difference between vegetated and unvegetated regions of a surface water body. This temperature difference will promote an exchange flow between the vegetation and open water. Drag associated with the submerged portion of the plants modifies this exchange, specifically, changing the dominant velocity scale. Scaling analysis predicts several distinct flow regimes, including inertia-dominated, drag-dominated and energy-limiting regimes. After a constant heat source is initiated, the flow is initially inertial, but quickly transitions to the drag-dominated regime. The energy-limiting regime is not likely to occur in the presence of rooted vegetation. Laboratory experiments describe the exchange flow and confirm the scaling analysis. Particle Imaging Velocimetry (PIV) was used to quantify the velocity field. Once the exchange flow enters the drag-dominated regime, the intrusion velocity uV is steady. The intrusion velocity decreases with increasing density of vegetation. The thickness of the intruding layer is set by the length scale of light penetration. 
520 |a National Science Foundation (U.S.) (Grant EAR0509658) 
546 |a en_US 
655 7 |a Article 
773 |t Journal of Fluid Mechanics