2015
DOI: 10.1051/proc/201448015
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Numerical simulation of the dynamics of sedimentary river beds with a stochastic Exner equation

Abstract: Abstract. At the scale of a river reach, the dynamics of the river bed is typically modelled by Exner equation (conservation of the solid mass) with an empirical solid flux of transported sediments, which is a simple deterministic algebraic formula function of i) the sediment physical characteristics (size and mass) and of ii) the averaged hydrodynamical description of the ambient water flow. This model has proved useful, in particular through numerical simulations, for hydraulic engineering purposes (like est… Show more

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Cited by 7 publications
(7 citation statements)
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References 39 publications
(45 reference statements)
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“…We have also illustrated with examples that the error created in using the advection‐diffusion equation for computing mean particle activity is small except in regions marked by sharp variations in the particle activity or activity gradients. Similar observations were made with the stochastic Burgers equation, a nonlinear equation that is close to the advection‐diffusion equation and in which particle activity is replaced by velocity: the solution to which the scheme converges depends on the mesh size [ Hairer and Voss , ] and velocity discontinuities are smoothed out even in the absence of diffusive terms [ Audusse et al , ]. This peculiar behavior of stochastic advection seems to be a common feature of stochastic partial differential equations (as the topic is quite recent, we may miss the broader view).…”
Section: Discussionmentioning
confidence: 54%
“…We have also illustrated with examples that the error created in using the advection‐diffusion equation for computing mean particle activity is small except in regions marked by sharp variations in the particle activity or activity gradients. Similar observations were made with the stochastic Burgers equation, a nonlinear equation that is close to the advection‐diffusion equation and in which particle activity is replaced by velocity: the solution to which the scheme converges depends on the mesh size [ Hairer and Voss , ] and velocity discontinuities are smoothed out even in the absence of diffusive terms [ Audusse et al , ]. This peculiar behavior of stochastic advection seems to be a common feature of stochastic partial differential equations (as the topic is quite recent, we may miss the broader view).…”
Section: Discussionmentioning
confidence: 54%
“…It bears strong analogies with but remains differ from that of Birnir et al [6]. Let us also mention a few remote works that rest upon a similar coupling philosophy but the scales of which are much smaller than ours: Delestre et al [9] on rainwater overland-flows, Cordier et al [8] on bedload transport, and Audusse et al [2] on sedimentary river beds.…”
Section: Introductionsupporting
confidence: 56%
“…Nevertheless, we observe that the preconditioner choice leads to important changes in the computational time. In our case, it is better to use ILU (2) or ILU (3). For stronger preconditioning methods, the cost of each iteration becomes too important to gain in efficiency.…”
Section: Delta Evolutionmentioning
confidence: 99%
“…Indeed, in real-world scenarios, water flow is rarely uniform as a result of the complex interplay between bed morphology, hydrodynamics, and sediment transport. As a consequence, stochastic models must be coupled with governing equations for the water phase (e.g., the shallow water equations), a task that raises numerous theoretical and computational problems [Bohorquez and Ancey, 2015;Audusse et al, 2015]. One of these problems is that existing stochastic models introduce a number of parameters (e.g., the particle diffusivity, the entrainment and deposition rates) without specifying how they depend on water flow.…”
Section: Introductionmentioning
confidence: 99%