This issuePrevious ArticleExistence of a weak solution for a quasilinear wave equation with boundary conditionNext ArticleModified wave operators for the Hartree equation with data, image and convergence in the same space
The Lagrangian averaged Euler equations as the short-time inviscid limit of the Navier–Stokes equations with Besov class data in $\mathbb{R}^2$
We compare the vorticity corresponding to a solution of the Lagrangian
averaged Euler equations on the plane to a solution of the Navier–Stokes equation with the same initial data, assuming that the averaged Euler
potential vorticity is in a certain Besov class of regularity. Then the averaged
Euler vorticity stays close to the Navier–Stokes vorticity for a short interval of
time as the respective smoothing parameters tend to zero with natural scaling.