1992
DOI: 10.1051/m2an/1992260708551
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Some estimates for the anisotropic Navier-Stokes equations and for the hydrostatic approximation

Abstract: Some estimates for the anisotropic Navier-Stokes equations and for the hydrostatic approximation RAIRO-Modélisation mathématique et analyse numérique, tome 26, n o 7 (1992), p. 855-865. © AFCET, 1992, tous droits réservés. L'accès aux archives de la revue « RAIRO-Modélisation mathématique et analyse numérique » implique l'accord avec les conditions générales d'utilisation (http://www.numdam.org/legal.php). Toute utilisation commerciale ou impression systéma… Show more

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Cited by 60 publications
(70 citation statements)
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“…In these works, compactness method is used to obtain the velocity u in a space with the restriction ∇ · u = 0 and the pressure is recovered, in the latter part of the argument, by a specific De Rham's lemma on the surface. In domains without sidewalls, the existence of a weak solution is obtained as a consequence of a limit process applied to the Navier-Stokes equations with anysotropic viscosity when the ratio depth over horizontal diameter (of the domain) tends to zero, see Besson-Laydi [5] for the stationary case and Azerad-Guillén [6] for the evolution case. Finally, the existence of a weak solution in domains without sidewalls can be proved by internal approximation arguments: a mixed (velocity-pressure) variational formulation of the stationary problem is approximated by a conform Finite Element method in Chacón-Guillén [7] and a semi-discretization in time of the evolution problem is proved that converges to continuous problem in Guillén-Redondo [8,9].…”
Section: Introductionmentioning
confidence: 99%
“…In these works, compactness method is used to obtain the velocity u in a space with the restriction ∇ · u = 0 and the pressure is recovered, in the latter part of the argument, by a specific De Rham's lemma on the surface. In domains without sidewalls, the existence of a weak solution is obtained as a consequence of a limit process applied to the Navier-Stokes equations with anysotropic viscosity when the ratio depth over horizontal diameter (of the domain) tends to zero, see Besson-Laydi [5] for the stationary case and Azerad-Guillén [6] for the evolution case. Finally, the existence of a weak solution in domains without sidewalls can be proved by internal approximation arguments: a mixed (velocity-pressure) variational formulation of the stationary problem is approximated by a conform Finite Element method in Chacón-Guillén [7] and a semi-discretization in time of the evolution problem is proved that converges to continuous problem in Guillén-Redondo [8,9].…”
Section: Introductionmentioning
confidence: 99%
“…It is then natural to perform the geometrical scaling z = z ε /ε (see [AG01,BL92]), obtaining the adimensional domain (figure 1):…”
Section: Preliminaries and Problem Settingmentioning
confidence: 99%
“…Equations (11)-(13) can be obtained as limit of the anisotropic Navier-Stokes equations (5)-(7) when ε tends to zero. This fact is justified on rigorous mathematical grounds in [BL92,AG01]. Many works about existence and regularity results of (11)-(13) are based on replacing this problem by the next (equivalent) reduced problem: find u : Ω × (0, T ) → R 2 , the horizontal velocity and p s : S × (0, T ) → R an (artificial) surface pressure, satisfying…”
Section: Preliminaries and Problem Settingmentioning
confidence: 99%
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“…one in which the horizontal dimension is very large compared with the vertical one, the hydrostatic approximation is the basic model. This model is obtained through a limit process from the anisotropic stationary Navier-Stokes equations and it is studied as such by Besson and Laydi in [2] and by Bresch and Simon in [3]. Several codes have also been developed to solve this problem [15].…”
Section: Introductionmentioning
confidence: 99%