On possible isolated blow-up phenomena of the 3D-Navier-Stokes equation and a regularity criterion in terms of supercritical function space condition and smoothness condition along the streamlines

Details On possible isolated blow-up phenomena of the 3D-Navier-Stokes equation and a regularity criterion in terms of supercritical function space condition and smoothness condition along the streamlines On possible isolated blow-up phenomena of the 3D-Navier-Stokes equation and a regularity criterion in terms of supercritical function space condition and smoothness condition along the streamlines

2010-11-26

arxiv.org/abs/1011.5863v1

Mathematics

Analysis of PDEs

Scientific paper

The first goal of our paper is to give a new type of regularity criterion for solutions $u$ to Navier-Stokes equation in terms of some supercritical function space condition $u \in L^{\infty}(L^{\alpha ,*})$ (with $\frac{3}{4}(17^{\frac{1}{2}} -1)< \alpha < 3 $) and some exponential control on the growth rate of $\dv (\frac{u}{|u|})$ along the streamlines of u. This regularity criterion greatly improves the previous one in \cite{smoothnesscriteria}. The proof leading to the regularity criterion of our paper basically follows the one in \cite{smoothnesscriteria}. However, we also point out that totally new idea which involves the use of the new supercritical function space condition is necessary for the success of our new regularity criterion in this paper. The second goal of our paper is to construct a divergence free vector field $u$ within a flow-invariant tubular region with increasing twisting of streamlines towards one end of a bundle of streamlines. The increasing twisting of streamlines is controlled in such a way that the associated quantities $\|u\|_{L^{\alpha}}$ and $\|\dv(\frac{u}{|u|})\|_{L^{6}}$ blow up while preserving the finite energy property $u\in L^{2}$ at the same time. The purpose of such a construction is to demonstrate the necessity to go beyond the scope covered by some previous regularity criteria such as \cite{Vasseur2} or \cite{Esca}.

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