On the localization of the magnetic and the velocity fields in the equations of magnetohydrodynamics

Studying approximations deduced from a Large Eddy Simulations model, we focus our attention in passing to the limit in the equation for the vorticity.. Generally speaking, if E(X) is

The aim of this work is to present some strategies to solve numerically controllability problems for the two-dimensional heat equation, the Stokes equations and the

§5, existence of very weak solution for the Navier-Stokes system is obtained, using a fixed point technique over the Oseen system, first for the case of small data and then

As it is well known, in the deterministic case, global existence of weak (in the PDE sense) solutions and uniqueness of strong solutions hold for the Navier-Stokes equations.. In

Galilei group has no superfluous components, and hence requires no wave- equation other than the orbital condition E = p2/2m, which is just the Schrödinger

– (1) Condition (1.1) appearing in the statement of Theorem 1 should be understood as a nonlinear smallness condition on the initial data: the parameter A, measuring through (H1)

TEMAM, Local existence of C~ solutions of the Euler equations of incompressible perfect fluids, in Proc. TEMAM, Navier-Stokes Equations and Nonlinear Functional Analysis,

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