The Structure of the Shear Layer in Flows over Rigid and Flexible Canopies

Flume experiments were conducted with rigid and flexible model vegetation to study the structure of coherent vortices (a manifestation of the Kelvin–Helmholtz instability) and vertical transport in shallow vegetated shear flows. The vortex street in a vegetated shear layer creates a pronounced oscillation in the velocity profile, with the velocity near the top of a model canopy varying by a factor of three during vortex passage. In turn, this velocity oscillation drives the coherent waving of flexible canopies. Relative to flows over rigid vegetation, the oscillation in canopy geometry has the effect of decreasing the amount of turbulent vertical momentum transport in the shear layer. Using a waving plant to determine phase in the vortex cycle, each vortex is shown to consist of a strong sweep at its front (during which the canopy is most deflected), followed by a weak ejection at its rear (when the canopy height is at a maximum). Whereas in unobstructed mixing layers the vortices span the entire layer, they encompass only 70% of the flexibly obstructed shear layer studied here.

[1]  M. Raupach,et al.  Conditional statistics of Reynolds stress in rough-wall and smooth-wall turbulent boundary layers , 1981, Journal of Fluid Mechanics.

[2]  G. Katul,et al.  A Note On The Contribution Of Dispersive Fluxes To Momentum Transfer Within Canopies , 2004 .

[3]  J. Finnigan,et al.  Coherent eddies and turbulence in vegetation canopies: The mixing-layer analogy , 1996 .

[4]  J. Finnigan Turbulence in plant canopies , 2000 .

[5]  H. Nepf,et al.  Mixing layers and coherent structures in vegetated aquatic flows , 2002 .

[6]  Marco Ghisalberti,et al.  Mass Transport in Vegetated Shear Flows , 2005 .

[7]  H. Nepf,et al.  Observations of particle capture on a cylindrical collector: Implications for particle accumulation and removal in aquatic systems , 2004 .

[8]  Syunsuke Ikeda,et al.  Three-Dimensional Organized Vortices above Flexible Water Plants , 1996 .

[9]  R. Chevray,et al.  Vortex dynamics in a plane, moderate-Reynolds-number shear layer , 1990, Journal of Fluid Mechanics.

[10]  Robert D. Moser,et al.  Direct Simulation of a Self-Similar Turbulent Mixing Layer , 1994 .

[11]  F. Short,et al.  Hydrodynamically induced synchronous waving of seagrasses: ‘monami’ and its possible effects on larval mussel settlement , 1996 .

[12]  C. Norberg Flow around a Circular Cylinder: Aspects of Fluctuating Lift , 2001 .

[13]  S. J. Kline,et al.  Combined dye-streak and hydrogen-bubble visual observations of a turbulent boundary layer , 1974, Journal of Fluid Mechanics.

[14]  James M. Wallace,et al.  The wall region in turbulent shear flow , 1972, Journal of Fluid Mechanics.

[15]  G. Edgar The influence of plant structure on the species richness, biomass and secondary production of macrofaunal assemblages associated with Western Australian seagrass beds , 1990 .

[16]  Enrique R. Vivoni,et al.  Flow structure in depth-limited, vegetated flow , 2000 .

[17]  Luca Ridolfi,et al.  The Effect of Vegetation Density on Canopy Sub-Layer Turbulence , 2004 .

[18]  Enrique Rafael Vivoni-Gallart,et al.  Turbulence structure of a model seagrass meadow , 1998 .

[19]  R. Shaw,et al.  Observation of organized structure in turbulent flow within and above a forest canopy , 1989 .

[20]  Chih-Ming Ho,et al.  Perturbed Free Shear Layers , 1984 .

[21]  A. Roshko,et al.  On density effects and large structure in turbulent mixing layers , 1974, Journal of Fluid Mechanics.

[22]  A. Ōkubo,et al.  Reduced mixing in a marine macrophyte canopy , 1993 .

[23]  M. Novak,et al.  Wind Tunnel And Field Measurements Of Turbulent Flow In Forests. Part I: Uniformly Thinned Stands , 2000 .

[24]  Marco Ghisalberti,et al.  The limited growth of vegetated shear layers , 2004 .

[25]  B. White Momentum and mass transport by coherent structures in a shallow vegetated shear flow , 2006 .