Dynamical Behavior for the Solutions of the Navier-Stokes Equation

preprint2016arXivOpen access

Abstract

We study the Cauchy problem for the incompressible Navier-Stokes equations (NS) in three and higher spatial dimensions: \begin{align} u_t -Δu+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<p≤∞d <p \leq \infty, ∥u(t)∥p≳(T−t)−(1−d/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 d≤p≤∞d\leq p\leq \infty for the blowup mild solution. On the other hand, if the Fourier support has the form supp u0^⊂{ξ∈Rn:ξ1≥L}{\rm supp} \ \widehat{u_0} \subset \{ξ\in \mathbb{R}^n: ξ_1\geq L \} and ∥u0∥∞≪L\|u_0\|_{\infty} \ll L for some L>0L >0, then \eqref{NSa} has a unique global solution u∈C(R+,L∞)u\in C(\mathbb{R}_+, L^\infty). Finally, if the blowup rate is of type I: ∥u(t)∥p∼(T−t)−(1−d/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 ΦΦ for which $$ \inf \{\limsup_{t \to T}(T-t)^{(1-3/p)/2}\|u(t)\|_{L^p_x}: \ u\in C([0,T); L^p) \mbox{\ solves \eqref{NSa}}\} $$ is attainable at some Φ∈L∞(0,T; B˙p/2,∞−1+6/p)Φ\in L^\infty (0,T; \ \dot B^{-1+6/p}_{p/2,\infty}).

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