An empirical model of aeolian dune lee-face airflow

Airflow data, gathered over dunes ranging from 60-m tall complex-crescentic dunes to 2-m tall simplecrescentic dunes, were used to develop an empirical model of dune lee-face airflow for straight-crested dunes. The nature of lee-face flow varies and was found to be controlled by the interaction of at least three factors (dune shape, the incidence angle between the primary wind direction and the dune brinkline and atmospheric thermal stability). Three types of lee-face flow (separated, attached and deflected along slope, or attached and undeflected) were found to occur. Separated flows, characterized by a zone of low-speed (0–3O% of crestal speed) back-eddy flow, typically occur leeward of steep-sided dunes in transverse flow conditions. Unstable atmospheric thermal stability also favours flow separation. Attached flows, characterized by higher flow speeds (up to 84% of crestal speed) that are a cosine function of the incidence angle, typically occur leeward of dunes that have a lower average lee slope and are subject to oblique flow conditions. Depending on the slope of the lee face, attached flow may be either deflected along slope (lee slopes greater than about 20°), or have the same direction as the primary flow (lee slopes less than about 20°). Neutral atmospheric thermal stability also favours flow attachment. As each of the three types of lee-face flow is defined by a range of wind speeds and directions, the nature of lee-face flow is intimately tied to the type of aeolian depositional process (i.e. wind ripple or superimposed dune migration, grainflow, or grainfall) that occurs on the lee slope and the resulting pattern of dune deposits. Therefore, the model presented in this paper can be used to enhance the interpretation of palaeowind regime and dune type from aeolian cross-strata.

[1]  J. R. Allen Sedimentary structures, their character and physical basis , 1982 .

[2]  William G. Nickling,et al.  The relationship of weather types to dust storm generation in Arizona (1965–1980) , 1986 .

[3]  D. Tritton,et al.  Physical Fluid Dynamics , 1977 .

[4]  G. D. Raithby,et al.  The Askervein hill project: A finite control volume prediction of three-dimensional flows over the hill , 1987 .

[5]  Alan D. Howard,et al.  Effect of slope on the threshold of motion and its application to orientation of wind ripples , 1977 .

[6]  B. Hand,et al.  Leeside Sediment Fallout Patterns and the Stability of Angular Bedforms , 1988 .

[7]  J. Allen Simple models for the shape and symmetry of tidal sand waves: (2) Dynamically stable symmetrical equilibrium forms , 1982 .

[8]  R. Folk Longitudinal dunes of the northwestern edge of the Simpson Desert , 1971 .

[9]  Robert A. Brown Longitudinal instabilities and secondary flows in the planetary boundary layer: A review , 1980 .

[10]  P. Mason,et al.  Atmospheric flow over a succession of nearly two‐dimensional ridges and valleys , 1984 .

[11]  N. Lancaster Variations in wind velocity and sand transport on the windward flanks of desert sand dunes , 1985 .

[12]  J. Hunt,et al.  Turbulent wind flow over a low hill , 1975 .

[13]  G. Kocurek,et al.  Interdune areas of the back-island dune field, North Padre Island, Texas , 1984 .

[14]  Robert P. Sharp,et al.  Kelso Dunes, Mojave Desert, California , 1966 .

[15]  M. L. Sweet,et al.  Algodones dune field of southeastern California: case history of a migrating modern dune field , 1988 .

[16]  Cincinnati WORKBOOK OF ATMOSPHERIC DISPERSION ESTIMATES , 1970 .

[17]  D. Inman,et al.  Coastal Sand Dunes of Guerrero Negro, Baja California, Mexico , 1966 .

[18]  G. Kocurek,et al.  A preliminary study of the dynamics of a modern draa , 1988 .

[19]  R. Bagnold,et al.  The Physics of Blown Sand and Desert Dunes , 1941 .

[20]  G. Kocurek,et al.  Climbing Zibars of the Algodones , 1986 .

[21]  H. Tsoar,et al.  Dynamic processes acting on a longitudinal (seif) sand dune , 1983 .

[22]  V. Cornish On the Formation of Sand-Dunes , 1897 .

[23]  E. F. Bradley An experimental study of the profiles of wind speed, shearing stress and turbulence at the crest of a large hill , 1980 .

[24]  B. Richmond,et al.  Daily cycles in coastal dunes , 1988 .

[25]  J. Walmsley,et al.  The Askervein Hill Project: Mean wind variations at fixed heights above ground , 1988 .

[26]  R. Folk Rollers and ripples in sand, streams and sky: rhythmic alteration of transverse and longitudinal vortices in three orders , 1976 .

[27]  Edwin D. McKee,et al.  STRUCTURES OF DUNES AT WHITE SANDS NATIONAL MONUMENT, NEW MEXICO (AND A COMPARISON WITH STRUCTURES OF DUNES FROM OTHER SELECTED AREAS)1 , 1966 .

[28]  W. Cooper Coastal sand dunes of Oregon and Washington , 1958 .

[29]  S. Hanna The Formation of Longitudinal Sand Dunes by Large Helical Eddies in the Atmosphere , 1969 .

[30]  J. Hardisty,et al.  Evidence for a new sand transport process from experiments on Saharan dunes , 1988, Nature.

[31]  J. H. Hoyt Air and Sand Movements to the Lee of DUNES1 , 1966 .

[32]  S. R. McLean,et al.  A Model for Flow Over Two‐Dimensional Bed Forms , 1986 .

[33]  Nicholas Lancaster,et al.  The dynamics of star dunes: an example from the Gran Desierto , 1989 .

[34]  The Flow in the Planetary Boundary Layer , 1983 .

[35]  P. Taylor,et al.  A numerical model of flow over sand waves in water of finite depth , 1981 .