Equivalent Roughness Height for Plane Bed under Steady Flow

This paper presents a new relationship between the roughness height and the main hydrodynamic and sediment parameters for plane beds under steady current conditions. In order to derive such a formula, a large data base involving plane-bed experiments was compiled from previous investigations and analyzed. Comparisons between the data and different existing predictive formulas for the bed roughness obtained from the literature were also made. A relationship with the Shields parameter only, which is commonly proposed, appeared to be insufficient. The roughness was also found to be a function of a Froude number and a dimensionless settling velocity. A critical Shields parameter was identified up to which the equivalent roughness ratio is proportional to the Shields parameter. The new empirical equation that was developed yields the best results for all conditions investigated, and should improve the understanding of the total shear stress.

[1]  Maurice J. Duncan,et al.  Relatively Rough Flow Resistance Equations , 2002 .

[2]  M. Selim Yalin,et al.  Mechanics of sediment transport , 1972 .

[3]  P. J. Whiting,et al.  Boundary Shear Stress and Roughness Over Mobile Alluvial Beds , 1990 .

[4]  Graeme M. Smart,et al.  Sediment Transport Formula for Steep Channels , 1984 .

[5]  L. Rijn Principles of sediment transport in rivers, estuaries and coastal seas , 1993 .

[6]  Joe C. Willis,et al.  LABORATORY STUDY OF TRANSPORT OF FINE SAND , 1972 .

[7]  Walter H. Graf,et al.  Uniform flow in open channels with movable gravel bed , 1994 .

[8]  J. W. Kamphuis,et al.  DETERMINATION OF SAND ROUGHNESS FOR FIXED BEDS , 1974 .

[9]  Kenneth C. Wilson,et al.  Bed-Load Transport at High Shear Stress , 1966 .

[10]  R. Soulsby Dynamics of marine sands : a manual for practical applications , 1997 .

[11]  D. Rickenmann Hyperconcentrated Flow and Sediment Transport at Steep Slopes , 1991 .

[12]  M. Selim Yalin CHAPTER 1 – FUNDAMENTALS , 1992 .

[13]  Vito Ferro,et al.  Flow Velocity Profiles in Gravel‐Bed Rivers , 1994 .

[14]  C. H. Hembree,et al.  Computations of Total Sediment Discharge, Niobrara River near Cody, Nebraska , 1954, Science.

[15]  D. B. Simons,et al.  Summary of alluvial channel data from flume experiments, 1956-61 , 1966 .

[16]  Weiming Wu,et al.  Movable bed roughness in alluvial rivers , 1999 .

[17]  G. Smart Turbulent Velocity Profiles and Boundary Shear in Gravel Bed Rivers , 1999 .

[18]  H. Schlichting Boundary Layer Theory , 1955 .

[19]  R. Soulsby Dynamics of marine sands , 1997 .

[20]  J. F. A. Sleath,et al.  Sea bed mechanics , 1984 .

[21]  J. Ahrens A Fall-Velocity Equation , 2000 .

[22]  J. K. Culbertson,et al.  Summary of alluvial-channel data from Rio Grande conveyance channel, New Mexico, 1965-69 , 1972 .

[23]  G. P. Williams Flume width and water depth effects in sediment-transport experiments , 1970 .

[24]  Kenneth C. Wilson,et al.  Mobile‐Bed Friction at High Shear Stress , 1989 .

[25]  Bruce W. Melville,et al.  Initiation of Bed Forms on a Flat Sand Bed , 1996 .

[26]  Jørgen Fredsøe,et al.  Velocity and concentration profiles in sheet-flow layer of movable bed , 1996 .

[27]  William R. Brownlie,et al.  Compilation of alluvial channel data : Laboratory and field , 1981 .

[28]  Kenneth C. Wilson,et al.  Analysis of Bed‐Load Motion at High Shear Stress , 1987 .

[29]  P. Julien,et al.  UPPER-REGIME PLANE BED , 1998 .

[30]  Kenneth C. Wilson,et al.  Motion of Contact‐Load Particles at High Shear Stress , 1992 .

[31]  M. D. Groot,et al.  Hyperconcentrated Sand‐Water Mixture Flows Over a Flat Bed , 1990 .

[32]  Van Rijn,et al.  Sediment transport; Part I, Bed load transport , 1984 .

[33]  Vladimir Nikora,et al.  Turbulence Characteristics of New Zealand Gravel-Bed Rivers , 1997 .