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Dynamical Behavior for the Solutions of the Navier-Stokes Equation

Analysis of PDEs 2016-08-25 v1

Abstract

We study the Cauchy problem for the incompressible Navier-Stokes equations (NS) in three and higher spatial dimensions: \begin{align} u_t -\Delta u+u\cdot \nabla u +\nabla p=0, \ \ {\rm div} u=0, \ \ u(0,x)= u_0(x). \label{NSa} \end{align} Leray and Giga obtained that for the weak and mild solutions uu of NS in Lp(Rd)L^p(\mathbb{R}^d) which blow up at finite time T>0T>0, respectively, one has that for d<pd <p \leq \infty, u(t)p(Tt)(1d/p)/2,  0<t<T. \|u(t)\|_p \gtrsim ( T-t )^{-(1-d/p)/2}, \ \ 0< t<T. We will obtain the blowup profile and the concentration phenomena in Lp(Rd)L^p(\mathbb{R}^d) with dpd\leq p\leq \infty for the blowup mild solution. On the other hand, if the Fourier support has the form supp u0^{ξRn:ξ1L}{\rm supp} \ \widehat{u_0} \subset \{\xi\in \mathbb{R}^n: \xi_1\geq L \} and u0L\|u_0\|_{\infty} \ll L for some L>0L >0, then \eqref{NSa} has a unique global solution uC(R+,L)u\in C(\mathbb{R}_+, L^\infty). Finally, if the blowup rate is of type I: u(t)p(Tt)(1d/p)/2, for 0<t<T<, d<p< \|u(t)\|_p \sim ( T-t )^{-(1-d/p)/2}, \ for \ 0< t<T<\infty, \ d<p<\infty in 3 dimensional case, then we can obtain a minimal blowup solution Φ\Phi for which inf{lim suptT(Tt)(13/p)/2u(t)Lxp: uC([0,T);Lp)\mbox solves\eqrefNSa} \inf \{\limsup_{t \to T}(T-t)^{(1-3/p)/2}\|u(t)\|_{L^p_x}: \ u\in C([0,T); L^p) \mbox{\ solves \eqref{NSa}}\} is attainable at some ΦL(0,T; B˙p/2,1+6/p)\Phi \in L^\infty (0,T; \ \dot B^{-1+6/p}_{p/2,\infty}).

Keywords

Cite

@article{arxiv.1608.06680,
  title  = {Dynamical Behavior for the Solutions of the Navier-Stokes Equation},
  author = {Kuijie Li and Tohru Ozawa and Baoxiang Wang},
  journal= {arXiv preprint arXiv:1608.06680},
  year   = {2016}
}

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