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Open AccessJournal ArticleDOI

Hydrodynamic processes, sediment erosion mechanisms, and Reynolds-number-induced scale effects in an open channel bend of strong curvature with flat bathymetry

TLDR
In this paper, the role of coherent flow structures, how these structures contribute to shear stresses and the capacity of the flow to pick up sediment at the boundaries, and on changes resulting from increasing the Reynolds number between typical values for laboratory model studies and for field conditions were investigated with eddy-resolving numerical simulations.
Abstract
[1] Sharply curved open channel flow with a flat bed is investigated with eddy-resolving numerical simulations that complement laboratory experiments. The focus is on the role of coherent flow structures, how these structures contribute to shear stresses and the capacity of the flow to pick up sediment at the boundaries, and on changes resulting from increasing the Reynolds number between typical values for laboratory model studies and for field conditions. In sharply curved bends, secondary flow leads to a transverse component of the bed shear stress that is of comparable magnitude as the streamwise component. Just downstream of the bend entrance, the locus of highest velocities migrates outward and separates from the inner bank. A highly energetic thin shear layer containing large-scale eddies develops at the interface between the core of high streamwise velocities and the retarded fluid moving close to the inner bank. Highly energetic Streamwise-Oriented Vortices (SOVs) develop in the zone of retarded flow. Turbulence, the boundary shear stress, and the sediment pickup capacity are considerably increased by the SOVs and the large-scale eddies inside the shear layer. These large-scale turbulent structures are amplified and become more coherent with increasing Reynolds number. The results indicate that flow processes in scaled laboratory flumes and natural rivers are qualitatively similar, although some quantitative Reynolds-number-induced scale effects exist. The paper also discusses application of several improved methods to estimate mean sediment pickup rates for flow in sharply curved bends. Such methods try to account in an approximate way for the effects of large-scale turbulence in numerical simulations that do not resolve these structures.

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Journal ArticleDOI

Effects of cylinder Reynolds number on the turbulent horseshoe vortex system and near wake of a surface-mounted circular cylinder

TL;DR: In this paper, the results of eddy-resolving simulations and supporting flow visualizations are investigated for the turbulent horseshoe vortex (HV) system and the near-wake flow past a circular cylinder mounted on a flat bed in an open channel.
Journal ArticleDOI

Large-eddy simulation in hydraulics: Quo Vadis?

TL;DR: The large-eddy simulation (LES) is used increasingly to address research and engineering problems of modern hydraulics as discussed by the authors and is used to simulate the large-scale motion of the flow and employs a model to account for the effects that small-scale turbulence imposes on large eddies.
Journal ArticleDOI

Numerical evaluation of the effects of planform geometry and inflow conditions on flow, turbulence structure, and bed shear velocity at a stream confluence with a concordant bed

TL;DR: In this paper, the effects of variations in inflow conditions and planform geometry on large-scale coherent flow structures and bed friction velocities at a stream confluence with natural bathymetry and concordant bed morphology were investigated.
Journal ArticleDOI

Influence of planform geometry and momentum ratio on thermal mixing at a stream confluence with a concordant bed

TL;DR: In this article, the effects of planform geometry and momentum flux ratio on thermal mixing at a stream confluence with concordant bed morphology are investigated based on numerical simulations that can capture the dynamics of large-scale turbulence.
Journal ArticleDOI

Hydrodynamics of mountain-river confluences and its relationship to sediment transport

TL;DR: In this article, eddy-resolving simulations based on laboratory experiments made in a live-bed model of a mountain-river confluence are used to provide a detailed description of flow hydrodynamics and implications for morphodynamics.
References
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MonographDOI

Turbulent Flows: FUNDAMENTALS

Eddies Stream, and Convergence Zones in Turbulent Flows

J. C. R. Hunt
TL;DR: In this article, a set of objective criteria were found which describe regions in which the streamlines circulate, converge, or diverge, and form high streams of high velocity flow.

The Bed-Load Function for Sediment Transportation in Open Channel Flows

Abstract: CONTENTS Page Introduction. 1 Approach to the problem. _ 3 Limitation of the bed-load function _ _ _ 4 The undetermined function 4 The alluvial stream. 5 The sediment mixture 6 Hydraulics of the alluvial channel. 7 The friction formula 7 The friction factor 8 Resistance of the bars 9 The laminar sublayer 10 The transition between hydraulically rough and smooth beds_ 12 The velocity fluctuations 13 Suspension 14 The transportation rate of suspended load 17 Integration of the suspended load. _ 17 Numerical integration of suspended load 19 Limit of suspension. 24 The bed layer 24 Practical calculation of suspended load___ ____ 25 Numerical example 26 Page Bed-load concept 29 Some constants entering the laws of bed-load motion: 31 The bed-load equation 32 The exchange time 33 The exchange probability 34 Determination of the probability V 35 Transition between bed load and. suspended load 38 The necessary graphs 40 Flume tests with sediment mixtures.. 42 Sample calculation of a river reachl 44 Choice of a river reach 45 Description of a river reach_____ 45 Application of procedure to Big Sand Creek, Miss 46 Discussion of calculations 60 Limitations of the method____ 65 Summary. 67 Literature cited 68 Appendix 69 List of symbols. 69 Work charts _ 71
Journal ArticleDOI

Detached-Eddy Simulation

TL;DR: This review discusses compelling examples, noting the visual and quantitative success of DES and its principal weakness is its response to ambiguous grids, in which the wall-parallel grid spacing is of the order of the boundary-layer thickness.
Book

The mechanics of scour in the marine environment

TL;DR: Scour Below Pipelines Scour around a single slender pile Scour Around a Group of Slender Piles Examples of More Complex Configurations ScourAround Large Piles Scouraround Breakwaters Scour at Seawalls Ship-Propeller Scour Impact of Liquefaction
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