2016
DOI: 10.1002/fld.4248
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SPH modelling of depth‐limited turbulent open channel flows over rough boundaries

Abstract: SUMMARYA numerical model based on the smoothed particle hydrodynamics method is developed to simulate depth-limited turbulent open channel flows over hydraulically rough beds. The 2D Lagrangian form of the Navier-Stokes equations is solved, in which a drag-based formulation is used based on an effective roughness zone near the bed to account for the roughness effect of bed spheres and an improved sub-particle-scale model is applied to account for the effect of turbulence. The sub-particle-scale model is constr… Show more

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Cited by 48 publications
(19 citation statements)
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“…κ = 0.41 is the Von Kármán constant, y is the distance from the wall, l max is a cutoff maximum value and the damping function in the first factor of the RHS avoids a non-physical growth of l near the free-surface when the particle distribution is irregular and the SPH evaluation of the gradient of a constant function departs sharply from zero: this function plays therefore a different role than the one of a wake function, such as the one included in the mixing-length model by [69] to simulate turbulent, open-channel uniform flows; the use of a wake function was not considered here because relevant turbulence effects occur mostly close to the hydraulic jump, where the flow conditions are in any case far from uniform; (2) A SPH version of the standard k-ε turbulence model by [70], in which µ T = c µ k 2 ε and the two equations for the turbulent kinetic energy k and for the turbulent dissipation rate ε are:…”
Section: Sph Numerical Methodsmentioning
confidence: 99%
“…κ = 0.41 is the Von Kármán constant, y is the distance from the wall, l max is a cutoff maximum value and the damping function in the first factor of the RHS avoids a non-physical growth of l near the free-surface when the particle distribution is irregular and the SPH evaluation of the gradient of a constant function departs sharply from zero: this function plays therefore a different role than the one of a wake function, such as the one included in the mixing-length model by [69] to simulate turbulent, open-channel uniform flows; the use of a wake function was not considered here because relevant turbulence effects occur mostly close to the hydraulic jump, where the flow conditions are in any case far from uniform; (2) A SPH version of the standard k-ε turbulence model by [70], in which µ T = c µ k 2 ε and the two equations for the turbulent kinetic energy k and for the turbulent dissipation rate ε are:…”
Section: Sph Numerical Methodsmentioning
confidence: 99%
“…Conversely, in the Marañon lowland, the Ecuadorian tributaries supply al- most 55 % of the water discharge and could significantly contribute to the river sediment load. The Napo River example (Laraque et al, 2009;Armijos et al, 2013) shows that the lowland part of the basin can be the main sediment source for these Ecuadorian tributaries. The river incision of this secondary source, and/or the Ecuadorian Andes, could provide coarser elements than the central Andean source does and explain why the ratios α are higher at BEL and REG than at the other sites.…”
Section: Index Concentration Relations Calibrated For Surface Index Smentioning
confidence: 99%
“…Thus, bedforms locally modify the ratio between the laminar and turbulent stresses, inducing different lifting profile shapes in the inner region (e.g. Kazemi et al, 2017) and causing the mixing length theory to fail in the overlap region.…”
Section: Estimation Of the Diffusivity Ratiomentioning
confidence: 99%