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Modélisation, analyse mathématique et simulations numériques de ...

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tel-00656013, version 1 - 3 Jan 2012<br />

Chapitre 2<br />

Derivation of a dynamic multilayer<br />

shallow water mo<strong>de</strong>l of<br />

approximation of free surface<br />

Navier-Stokes equations ; existence of<br />

local in time strong solution<br />

We propose a new simple approximation of the viscous primitive equations of the ocean<br />

including Coriolis force (2.1.1), by a multilayer shallow water type mo<strong>de</strong>l. Using a finite<br />

volume type discr<strong>et</strong>ization in the vertical direction, we show that our system is a consistent<br />

approximation of (2.1.1) and we compare it briefly with other multilayer shallow water type<br />

existing mo<strong>de</strong>ls. Next, existence and uniqueness of local in time strong solution is proved<br />

for the new mo<strong>de</strong>l.<br />

2.1 Introduction and Main Result<br />

The main goal of this work is to propose a simple and numerically efficient mo<strong>de</strong>l of<br />

geophysical flows such as large-scale ocean circulations. Many of these flows are generally<br />

<strong>de</strong>scribed by the incompressible Navier-Stokes equations with a free surface [137]. Due<br />

to the mathematical complexity of this system, different approximations are usually performed,<br />

which aim in particular at finding a compromise b<strong>et</strong>ween physical consistency<br />

and reasonable computational cost. Going beyond the Boussinesq approximation [159] we<br />

start our study by consi<strong>de</strong>ring an homogeneous fluid (water), with <strong>de</strong>nsity equal to one.<br />

Moreover we use the so-called hydrostatic approximation, that is we assume the pressure<br />

is hydrostatic and is not an unknown of the problem. Precisely, the <strong>de</strong>parture mo<strong>de</strong>l consists<br />

in the primitive equations of the ocean, given in the conservative form below. We<br />

use bold characters to indicate vector valued functions or variables. Hence the 3D velocity<br />

of the fluid, for which we separate the horizontal component and the vertical one as<br />

45

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