Instabilité non-linéaire transverse de solitons de l'équation d'Euler-Korteweg

At first sight, this may seems strange because Theorem 7.1 deals with large boundary layers and in some similar settings large boundary layers have in general a nonlinear behavior

In this work, we analyse the internal shear layer structures generated by the libration of an axisymmetric object in an unbounded fluid rotating at a rotation rate Ω ∗ using

For fluids with shear-rate dependent viscosity the base flow is no longer an exact solution of the Navier-Stokes equations, however, in the limit of large Reynolds number the

The second PML model we have proposed for the Euler linearized equations are based on the PML for the advective wave equation.. Thus, the PML for Euler inherits the properties from

Grand établissement sous tutelle de l'Education nationale Grande voie des vignes 92295 Châtenay Malabry

We want to improve the convergence result of [16] and show the global in time convergence of the weak solution of the system of rotating fluids towards the solution of a

Oh, Existence of semiclassical bound states of nonlinear Schrödinger equations with potentials of the class (V ) a , Comm. Oh, Stability of semiclassical bound states of

To apply this method to the Euler–Korteweg system, we face the added difficulty that solutions are thus far not known to exist around 1-dimensional travelling waves in 2D: the result