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Numerical simulation of turbulence and sediment transport of medium sand

Mark W. Schmeeckle
- 01 Jun 2014 - 
- Vol. 119, Iss: 6, pp 1240-1262
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TLDR
In this paper, a model of sand transport in water is produced by combining a turbulence-resolving large eddy simulation (LES) with a discrete element model (DEM) prescribing the motion of individual grains of medium sand.
Abstract
A model of sand transport in water is produced by combining a turbulence-resolving large eddy simulation (LES) with a discrete element model (DEM) prescribing the motion of individual grains of medium sand. The momentum effect of each particle on the fluid is calculated at the LES cell containing the particle, and the fluid velocity and pressure, interpolated to each particle center, is used to derive fluid force on each particle in the DEM. Eleven numerical experiments are conducted of an initially flat bed of particles. The experiments span a range of motion, from essentially no motion to vigorous suspension. Hydraulic roughness is found to increase abruptly at the transition from bed load to suspended load transport. Suspended sediment extracts momentum from the flow and decreases the rate of shear. Whereas, slightly higher in the flow, vertical drag by suspended grains damps turbulence and increases the rate of shear. Vertical sediment diffusivity and effective particle settling velocity are much smaller than is commonly assumed in suspended sediment models. The bed load experiments suggest that saltation by itself is a poor model of bed load sand transport. In contrast to expectations from saltation models, the peak bed load flux occurs at essentially the same level as the bed, and grains move slowly in frequent contact with other grains. Higher- and faster-moving bed load grains that can be considered to be in saltation represent a smaller portion of the total flux. Entrainment of bed load grains occurs in response to fluid penetration of the bed by high-vorticity turbulence structures embedded within broader high speed fluid regions referred to as a sweeps or high-speed wedges.

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Journal ArticleDOI

Onset of sediment transport is a continuous transition driven by fluid shear and granular creep.

TL;DR: A new phase diagram is proposed for sediment transport, where ‘bed load’ is a dense granular flow bounded by creep below and suspension above, where creep is characteristic of disordered solids and reminiscent of soil diffusion on hillslopes.
Journal ArticleDOI

A physical model for seismic noise generation by turbulent flow in rivers

TL;DR: In this paper, the authors proposed a forward model of seismic noise caused by turbulent flow and found that turbulent flow induced seismic noise operates at lower frequencies than bedload-induced noise, and the differences in the spectral signatures of turbulent flow-induced and bedload induced forces at the riverbed are significant enough that these two processes can be characterized independently using seismic records acquired at various distances from the river.
Journal ArticleDOI

SediFoam: A general-purpose, open-source CFD–DEM solver for particle-laden flow with emphasis on sediment transport

TL;DR: The development of a three-dimensional, massively parallel, and open-source CFD–DEM solver SediFoam is detailed, built based onopen-source solvers OpenFOAM and LAMMPS, and the parallel efficiency tests show that the scalability of SediBoat is satisfactory in the simulations using up to O ( 10 7 ) particles.
Journal ArticleDOI

The Physics of Sediment Transport Initiation, Cessation, and Entrainment Across Aeolian and Fluvial Environments

TL;DR: In this paper, the physics of sediment transport initiation, cessation, and capacity are reviewed with emphasis on recent consensus-challenging developments in sediment transport experiments, two-phase flow modeling, and the incorporation of granular physics' concepts.
Journal ArticleDOI

Formation of sediment patterns in channel flow: minimal unstable systems and their temporal evolution

TL;DR: In this paper, the authors investigated the phenomenon of sediment pattern formation in a channel flow by performing simulations which resolve all the relevant length and time scales of the problem, and found that the cutoff length for pattern formation lies in the range 75-100 times the particle diameter (3-4 times the clear fluid height).
References
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Journal Article

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Peter Cundall, +1 more
- 01 Jan 1979 - 
TL;DR: The distinct element method as mentioned in this paper is a numerical model capable of describing the mechanical behavior of assemblies of discs and spheres and is based on the use of an explicit numerical scheme in which the interaction of the particles is monitored contact by contact and the motion of the objects modelled particle by particle.
Journal ArticleDOI

A discrete numerical model for granular assemblies

Peter Cundall, +1 more
- 01 Mar 1979 - 
TL;DR: The distinct element method as mentioned in this paper is a numerical model capable of describing the mechanical behavior of assemblies of discs and spheres and is based on the use of an explicit numerical scheme in which the interaction of the particles is monitored contact by contact and the motion of the objects modelled particle by particle.
Journal ArticleDOI

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TL;DR: In this article, a new eddy viscosity model is presented which alleviates many of the drawbacks of the existing subgrid-scale stress models, such as the inability to represent correctly with a single universal constant different turbulent fields in rotating or sheared flows, near solid walls, or in transitional regimes.
Journal ArticleDOI

Equation of motion for a small rigid sphere in a nonuniform flow

TL;DR: In this paper, the forces on a small rigid sphere in a nonuniform flow are considered from first prinicples in order to resolve the errors in Tchen's equation and the subsequent modified versions that have since appeared.

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.
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