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River Flow 2004 2004
DOI: 10.1201/b16998-90
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Pressure fluctuations within subsurface gravel bed caused by turbulent open-channel flow

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Cited by 9 publications
(10 citation statements)
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“…The σ ≈ τ 0 dependence was mainly demonstrated for impermeable (continuous) smooth and rough beds. More recently, Detert et al (2004) reported similar results with σ ≈ (3-3.5)τ 0 for hydraulically rough flow over a multi-layered and homogeneous stratum of spherical particles of diameter 10 mm. Smart & Habersack (2007) showed that this dependence is also observed in gravel-bed rivers, and through their field data reported that σ ≈ 3τ 0 .…”
Section: Pressure Forces On Sediment Particles In Turbulent Open-chansupporting
confidence: 62%
See 1 more Smart Citation
“…The σ ≈ τ 0 dependence was mainly demonstrated for impermeable (continuous) smooth and rough beds. More recently, Detert et al (2004) reported similar results with σ ≈ (3-3.5)τ 0 for hydraulically rough flow over a multi-layered and homogeneous stratum of spherical particles of diameter 10 mm. Smart & Habersack (2007) showed that this dependence is also observed in gravel-bed rivers, and through their field data reported that σ ≈ 3τ 0 .…”
Section: Pressure Forces On Sediment Particles In Turbulent Open-chansupporting
confidence: 62%
“…It was found that σ D and σ L were 2-2.6 and 2.5-3.4 times τ 0 , respectively. While this link between bed shear stress and pressure fluctuations was first derived for smooth beds (Kraichnan 1956), the present results along with those reported by Detert et al (2004) and Smart & Habersack (2007) suggest a technique for estimating local boundary shear stress if instantaneous near-bed pressure measurements can be recorded for flows over rough granular beds. However, the exact flow mechanisms responsible for this link between τ 0 and σ p over rough beds remain to be identified and tested.…”
Section: Discussionmentioning
confidence: 54%
“…Since wood causes shedding vortices and enlarges turbulence intensity in the surface water [ Mutz , 2003], instream wood is likely to increase turbulent dispersion. However, turbulent pressure variations and dispersion in a porous bed are limited to approximately two to three times the roughness height of a porous bed [ Detert et al , 2004; Dittrich and Träbing , 1999]. Assuming that roughness height is the d 90 of the grain size distribution [ Schneider , 1998], the sediment layer that may have been affected by the exchange mechanism in the experiments was 1.7 to 2.3 mm deep.…”
Section: Discussionmentioning
confidence: 99%
“…Hydrodynamically induced flow can also be generated by boundary layer turbulence in open channel flow [e.g., Blois et al ., ], especially in gravels where pore water velocities near the bed interface can reach magnitudes in the order of 0.2 m s −1 [ Nagaoka and Ohgaki , ]. These flow velocities are generated by coherent flow structures in the turbulent boundary layer, as well as flow separation induced by bed‐topography, and may be expected to generate significant pressure gradients across the bed and into the pores beneath [ Detert et al ., ]. These flows result in intense turbulent fluctuations in the hyporheic flow within the pore spaces in the Brinkman layer (defined as the transition layer between the fully turbulent flow and the deeper groundwater Darcian flow, Goharzadeh et al .…”
Section: Introductionmentioning
confidence: 99%