Local Log-Law-of-the-Wall in Neutrally-Stratified Boundary-Layer Flows

It is well known that in a neutrally-stratified turbulent flow in a deep constant-stress layer above a flat surface,the horizontal mean velocity varies logarithmically with height (the so-called `log-law-of-the-wall').More recently, the same logarithmic law has also been foundin the presence of non-flat surfaces, where it governs thedynamics of the areally-averagedvelocity and involves renormalized effective parameters.Here, we analyze wind profiles over two-dimensional sinusoidal hillsobtained both from numerical simulations performed with a primitiveequation model and from wind-tunnel measurements. We showthat also the local velocity profiles behave to a verygood approximation logarithmically, for a distance from the surface of the order of the maximum hill height almost to the top of the boundary layer. Such alocal log-law-of-the-wall involves effective parameters smoothly depending on theposition along the underlying topography.This dependence looks very similar to the topography itself.

[1]  S. Belcher,et al.  The drag on an undulating surface induced by the flow of a turbulent boundary layer , 1993, Journal of Fluid Mechanics.

[2]  C. F. Ratto,et al.  Local law-of-the-wall in complex topography: a confirmation from wind tunnel experiments , 2001, physics/0103090.

[3]  P. J. Mason,et al.  On the parameterization of drag over small-scale topography in neutrally-stratified boundary-layer flow , 1989 .

[4]  Hans A. Panofsky,et al.  The geostrophic drag coefficient and the ‘effective’ roughness length , 1972 .

[5]  M. Athanassiadou,et al.  Neutral Flow Over A Series Of Rough Hills: A Laboratory Experiment , 2001 .

[6]  Nigel Wood,et al.  Large-Eddy Simulation Of Neutral Turbulent Flow Over Rough Sinusoidal Ridges , 2001 .

[7]  P. Taylor,et al.  Boundary-layer parametrization of drag over small-scale topography , 1995 .

[8]  J. Hunt,et al.  Turbulent shear flows over low hills , 1988 .

[9]  A. Townsend The Structure of Turbulent Shear Flow , 1975 .

[10]  W. Gong,et al.  Turbulent boundary-layer flow over fixed aerodynamically rough two-dimensional sinusoidal waves , 1996, Journal of Fluid Mechanics.

[11]  F. Hewer Non-Linear Numerical Model Predictions of Flow Over an Isolated Hill of Moderate Slope , 1998 .

[12]  Local log-law of the wall: numerical evidences and reasons , 2000, nlin/0010043.

[13]  E. F. Bradley,et al.  Boundary-layer flow over low hills , 1987 .

[14]  Andrea Mazzino,et al.  Comparison between the results of a new version of the AVACTA II atmospheric diffusion model and tracer experiments , 1997 .

[15]  P. Mason Atmospheric boundary layer flows: Their structure and measurement , 1995 .

[16]  W. Kustas,et al.  Wind profile constants in a neutral atmospheric boundary layer over complex terrain , 1986 .

[17]  P. Hignett,et al.  Estimates of effective surface roughness over complex terrain , 1994 .

[18]  Stefan Emeis Pressure Drag of Obstacles in the Atmospheric Boundary Layer , 1990 .

[19]  P. J. Mason,et al.  The formation of areally‐averaged roughness lengths , 1988 .

[20]  N. Wood,et al.  The Pressure force induced by neutral, turbulent flow over hills , 1993 .

[21]  Peter A. Taylor,et al.  Boundary-layer flow over topography : Impacts of the Askervein study , 1996 .

[22]  J. Holton An introduction to dynamic meteorology , 2004 .

[23]  Nigel Wood,et al.  Wind Flow Over Complex Terrain: A Historical Perspective and the Prospect for Large-Eddy Modelling , 2000, Boundary-Layer Meteorology.

[24]  M. G. Morselli,et al.  Boundary-layer flow over analytical two-dimensional hills: A systematic comparison of different models with wind tunnel data , 1993 .

[25]  P. Mason,et al.  Observations of boundary-layer structure over complex terrain , 1990 .