Flow through a very porous obstacle in a shallow channel

A theoretical model, informed by numerical simulations based on the shallow water equations, is developed to predict the flow passing through and around a uniform porous obstacle in a shallow channel, where background friction is important. This problem is relevant to a number of practical situations, including flow through aquatic vegetation, the performance of arrays of turbines in tidal channels and hydrodynamic forces on offshore structures. To demonstrate this relevance, the theoretical model is used to (i) reinterpret core flow velocities in existing laboratory-based data for an array of emergent cylinders in shallow water emulating aquatic vegetation and (ii) reassess the optimum arrangement of tidal turbines to generate power in a tidal channel. Comparison with laboratory-based data indicates a maximum obstacle resistance (or minimum porosity) for which the present theoretical model is valid. When the obstacle resistance is above this threshold the shallow water equations do not provide an adequate representation of the flow, and the theoretical model over-predicts the core flow passing through the obstacle. The second application of the model confirms that natural bed resistance increases the power extraction potential for a partial tidal fence in a shallow channel and alters the optimum arrangement of turbines within the fence.

[1]  H. Nepf,et al.  Vortex development behind a finite porous obstruction in a channel , 2011, Journal of Fluid Mechanics.

[2]  I. Eames,et al.  Numerical study of flow through and around a circular array of cylinders , 2011, Journal of Fluid Mechanics.

[3]  M. Oldfield,et al.  Application of linear momentum actuator disc theory to open channel flow , 2008 .

[4]  T. Nishino,et al.  Centred and staggered arrangements of tidal turbines , 2013, Journal of Fluid Mechanics.

[5]  C. Garrett,et al.  The efficiency of a turbine in a tidal channel , 2007, Journal of Fluid Mechanics.

[6]  P. Stansby,et al.  Modelling shallow-water low around pipe groups , 1996 .

[7]  E. Toro,et al.  Restoration of the contact surface in the HLL-Riemann solver , 1994 .

[8]  Akira Sase,et al.  Drag force due to vegetation in mangrove swamps , 1997 .

[9]  Yukie Tanino,et al.  Laboratory Investigation of Mean Drag in a Random Array of Rigid, Emergent Cylinders , 2008 .

[10]  R. Vennell Tuning turbines in a tidal channel , 2010, Journal of Fluid Mechanics.

[11]  Julien Lhomme,et al.  Two-dimensional shallow-water model with porosity for urban flood modelling , 2008 .

[12]  C. Wood,et al.  The Effect of Base Bleed on a Periodic Wake , 1964, Journal of the Royal Aeronautical Society.

[13]  H. Nepf,et al.  The wake structure behind a porous obstruction and its implications for deposition near a finite patch of emergent vegetation , 2012 .

[14]  N. Tanaka,et al.  Flow structures and drag characteristics of a colony-type emergent roughness model mounted on a flat plate in uniform flow , 2007 .

[15]  R. Willden,et al.  The efficiency of an array of tidal turbines partially blocking a wide channel , 2012, Journal of Fluid Mechanics.

[16]  Peter Stansby,et al.  A mixing-length model for shallow turbulent wakes , 2003, Journal of Fluid Mechanics.

[17]  G. Jackson Currents in the high drag environment of a coastal kelp stand off California , 1997 .

[18]  Peter Stansby Limitations of Depth-Averaged Modeling for Shallow Wakes , 2006 .

[19]  C. Garrett,et al.  Maximum power from a turbine farm in shallow water , 2013, Journal of Fluid Mechanics.

[20]  G. Jirka,et al.  Experimental study of plane turbulent wakes in a shallow water layer , 1995 .

[21]  R. Willden,et al.  Two-scale dynamics of flow past a partial cross-stream array of tidal turbines , 2013, Journal of Fluid Mechanics.

[22]  H. Nepf,et al.  Flow adjustment and interior flow associated with a rectangular porous obstruction , 2011, Journal of Fluid Mechanics.