Publication
On Some Weighted Stokes Problems. Application on Smagorinsky Models
Résumé
In this paper we study existence and uniqueness of weak solutions for some non-linear weighted Stokes problems using convex analysis. The characteri- zation of these considered equations is that the viscosity depends on the strain rate of the velocity field with a weight being a positive power of the distance to the boundary of the domain. These non-linear relations can be seen as a first approach of mixing-length eddy viscosity from turbulent modeling. A well known model is von Karman’s on which the viscosity depends on the square of the distance to the boundary of the domain. Numerical experiments conclude the work and show prop- erties from the theory.
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Proximité ontologique
Concepts associés (33)
Turbulence
vignette|Léonard de Vinci s'est notamment passionné pour l'étude de la turbulence. La turbulence désigne l'état de l'écoulement d'un fluide, liquide ou gaz, dans lequel la vitesse présente en tout point un caractère tourbillonnaire : tourbillons dont la taille, la localisation et l'orientation varient constamment. Les écoulements turbulents se caractérisent donc par une apparence très désordonnée, un comportement difficilement prévisible et l'existence de nombreuses échelles spatiales et temporelles.
Viscosité
La viscosité (du latin viscum, gui, glu) peut être définie comme l'ensemble des phénomènes de résistance au mouvement d'un fluide pour un écoulement avec ou sans turbulence. La viscosité diminue la liberté d'écoulement du fluide et dissipe son énergie. Deux grandeurs physiques caractérisent la viscosité : la viscosité dynamique (celle utilisée le plus généralement) et la seconde viscosité ou la viscosité de volume. On utilise aussi des grandeurs dérivées : fluidité, viscosité cinématique ou viscosité élongationnelle.
Apparent viscosity
In fluid mechanics, apparent viscosity (sometimes denoted η) is the shear stress applied to a fluid divided by the shear rate: For a Newtonian fluid, the apparent viscosity is constant, and equal to the Newtonian viscosity of the fluid, but for non-Newtonian fluids, the apparent viscosity depends on the shear rate. Apparent viscosity has the SI derived unit Pa·s (Pascal-second), but the centipoise is frequently used in practice: (1 mPa·s = 1 cP).
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