Stokes and Navier-Stokes equations with Navier boundary condition Equations de Stokes et de Navier-Stokes avec la condition de Navier

We also study the existence of weak solutions to the three-dimensional instationary Navier–Stokes equations for more regular data, but without any smallness assumption on the

a problem the unknown angular velocity co for the appropriate coordinate system in which the solution is stationary can be determined by the equilibrium

NIRENBERG, Partial regularity of suitable weak solutions of the Navier-Stokes equations. FRASCA, Morrey spaces and Hardy-Littlewood maximal

— We proved in Section 2 of [7] a local existence and uniqueness theorem (Theorem 2.2) for solutions of the Navier- Stokes equations with initial data in a space 7-^1 ^2,<5s ^

The interest in introducing the 0-(p approach in turbulence modelling is that (S) may be considered as a stabilization of the k-e model in the sense that we can state some

Mod` eles de fluide incompressible M´ ethodes de discr´ etisation M´ ethodes Euler/Lagrange M´ ethodes Vortex Bureau d’´ Etudes.. Calcul d’´ ecoulements par m´

We analyze the problem mainly using the Bhatnagar–Gross–Krook (also known as BGK) model, but some results based on the original Boltzmann equation will also be presented. Because of

Taking the duality method introduced by Lions & Magenes in [28] and Giga in [20] up again for open sets of class C ∞ (see also Necas [31] chapter 4 that consider the Hilbertian