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Rapid Increase in Suspended Load at High Bed Shear
When the dimensionless shear stress θ exceeds 0.8 a plane shear layer develops on the top of a granular bed. This layer is stabilized by the mixture density gradient within it. Its thickness typically increases linearly with θ , and so does the ratio of the effective roughness size to particle diame...
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Published in: | Journal of hydraulic engineering (New York, N.Y.) N.Y.), 2005-01, Vol.131 (1), p.46-51 |
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Main Author: | |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | When the dimensionless shear stress
θ
exceeds 0.8 a plane shear layer develops on the top of a granular bed. This layer is stabilized by the mixture density gradient within it. Its thickness typically increases linearly with
θ
, and so does the ratio of the effective roughness size to particle diameter,
ks
∕d
. If the ratio of shear velocity
U*
to particle fall velocity
Vf
is sufficiently large, the shear layer may be destabilized, giving a rapid increase in turbulent suspension. New closed-conduit experiments with
0.11
mm
sand show that for
U*∕
Vf
>6.5
the ratio
ks
∕d
has a pronounced increase above the typical shear-layer trend, and so does the suspended-load concentration (measured at the mid-height between the stationary bed and the top of the flow). These observations differ significantly from the sediment pick-up function in common use, indicating that the latter must be reconsidered. The present experiments also show a tie-in with hyperconcentrated flow as observed in the rivers of Northern China. |
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ISSN: | 0733-9429 1943-7900 |
DOI: | 10.1061/(ASCE)0733-9429(2005)131:1(46) |