Annihilation of slowly-decaying terms of Navier-Stokes flows by external forcing
Post-refereeing version. To appear in Nonlinearity
Résumé
The goal of this paper is to provide an algorithm that, for any sufficiently localised, divergence-free small initial data, explicitly constructs a localised external force leading to a rapidly dissipative solutions of the Navier-Stokes equations R n : namely, the energy decay rate of the flow will be forced to satisfy \( \|u(t)\|_ 2^2 = o(t^{ −(n+2)/2}) \) as \( t\to\infty \), which is beyond the usual optimal rate. An important feature of our construction is that this force can always be taken compactly supported in space-time, and its profile arbitrarily prescribed up to a spatial rescaling. Since the forcing term vanishes after a finite time interval, our result suggests that nontrivial interactions between the linear and nonlinear parts occur, annihilating all the slowly decaying terms contained in Miyakawa and Schonbek's asymptotic profiles.
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Commentaire : Ce pdf est la version preprint de l'article (version soumise à l'éditeur, avant peer-reviewing).
Commentaire : Ce pdf est la version preprint de l'article (version soumise à l'éditeur, avant peer-reviewing).