Vol. 254, No. 2, 2011

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Structure of solutions of 3D axisymmetric Navier–Stokes equations near maximal points

Zhen Lei and Qi S. Zhang

Vol. 254 (2011), No. 2, 335–344
Abstract

Let v be a solution of the axially symmetric Navier–Stokes equation. We determine the structure of a certain (possible) maximal singularity of v in the following sense. Let (x0,t0) be a point where the flow speed Q0 = |v(x0,t0)| is comparable with the maximum flow speed at and before time t0. We show, after a space-time scaling with the factor Q0 and the center (x0,t0), that the solution is arbitrarily close in Clocal2,1 norm to a nonzero constant vector in a fixed parabolic cube, provided that r0Q0 is sufficiently large. Here r0 is the distance from x0 to the z axis. Similar results are also shown to be valid if |r0v(x0,t0)| is comparable with the maximum of |rv(x,t)| at and before time t0. This mirrors a numerical result of Hou for the Euler equation: there exists a certain “calm spot” or depletion of vortex stretching in a region of high flow speed.

Keywords
Axisymmetric Navier–Stokes equations, structure of singularities
Mathematical Subject Classification 2010
Primary: 35Q30, 76D05
Milestones
Received: 16 February 2011
Revised: 16 September 2011
Accepted: 31 October 2011
Published: 27 February 2012
Authors
Zhen Lei
School of Mathematical Sciences
LMNS and Shanghai Key Laboratory for Contemporary Applied Mathematics
Fudan University
Shanghai 200433
China
Qi S. Zhang
Department of Mathematics
University of California
Riverside, CA 92521
United States