EDP Sciences / Société de Mathématiques Appliquées et Industrielles
Abstract
This is an Open Access article distributed under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0),
which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.In this work, we present a family of layer-averaged models for the Navier–Stokes equations.
For its derivation, we consider a layerwise linear vertical profile for the horizontal velocity component.
As a particular case, we also obtain layer-averaged models with the common layerwise constant approximation
of the horizontal velocity. The approximation of the derivatives of the velocity components is
set by following the theory of distributions to account for the discontinuities at the internal interfaces.
Several models has been proposed, depending on the order of approximation of an asymptotic analysis
respect to the shallowness parameter. Then, we obtain a hydrostatic model with vertical viscous effects,
a hydrostatic model where the pressure depends on the stress tensor, and fully non-hydrostatic models,
with a complex rheology. It is remarkable that the proposed models generalize plenty of previous
models in the literature. Furthermore, all of them satisfy an exact dissipative energy balance. We also
propose a model that is second-order accurate in the vertical direction thanks to a correction of the
shear stress approximation. Finally, we show how effective the layerwise linear approach is to notably
improve, with respect to the layerwise constant method, the approximation of the velocity profile for
some geophysical flows. Namely, a Newtonian fluid and some complex viscoplastic (dry granular and
Herschel–Bulkley) materials are considered