Abstract
In wind tunnel studies of aeolian transport, the number and position of pitot tubes are decided by the researcher, so that there are important variations in the computation ofU * between studies. Velocity measurements seldom are made very close to mobile surfaces because the tubes become blocked by drifting sand grains. This practice is fortuitous as demonstrated by recent selfregulatory models of saltation which indicate that fluid and grain-borne shear stress vary substantially within the lowest 0.01 m and application of the logarithmic law is therefore unsound. This study reports detailed velocity measurements which further suggest that no single logarithmic expression, based on fixed values of κ and τ, adequately represents the full wind profile which includes the inner saltation cloud above 0.01 m and the outer grain-free region of the boundary layer. A much improved fit over the logarithmic wind profile model is achieved with a square root relation, although there is no known physical basis for this specific form of power model. Relatively shallow boundary-layer development in wind tunnels forces the velocity gradient above the region of momentum extraction to attain exceptionally large values, uncommon in natural settings.
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Abbreviations
- U * :
-
shear velocity
- U *1 :
-
threshold shear velocity
- τ:
-
shear stress
- U z :
-
velocity atZ
- U 1z :
-
velocity atZ, standardized byU f
- U t :
-
threshold velocity atk′
- U f :
-
free-stream velocity
- D :
-
mean grain diameter
- ϕ:
-
unit of grain size (−log2 D)
- l 1 :
-
mixing length at unit height
- Z :
-
height above surface
- Z 0 :
-
roughness length
- k′:
-
focus height
- H :
-
wind tunnel height
- d :
-
height of the internal boundary layer
- α,c, C, D′:
-
empirical coefficients
- F :
-
Froude number
- F c :
-
Cole's wake function
- κ:
-
von Karman's constant
- p :
-
exponent
- C D :
-
drag coefficient
- g :
-
gravitational acceleration
- ∈y :
-
standard error of velocity estimate
- Q :
-
sediment flux
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All lengths in m, velocities in m s−1, and fluxes in kg m−1 s−1 unless otherwise stated. All velocities are time averaged. The bed condition is indicated by the additional subscripts:m (mobile) and s (stable).
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Neuman, C.M., Nickling, W.G. Momentum extraction with saltation: Implications for experimental evaluation of wind profile parameters. Boundary-Layer Meteorol 68, 35–50 (1994). https://doi.org/10.1007/BF00712663
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DOI: https://doi.org/10.1007/BF00712663