Stabilizing the long-time behavior of the forced Navier-Stokes and damped Euler systems by large mean flow

被引:3
|
作者
Cyranka, Jacek [1 ,5 ]
Mucha, Piotr B. [1 ]
Titi, Edriss S. [2 ,3 ]
Zgliczynski, Piotr [4 ]
机构
[1] Univ Warsaw, Inst Appl Math & Mech, Ul Banacha 2, PL-02097 Warsaw, Poland
[2] Texas A&M Univ, Dept Math, College Stn, TX 77843 USA
[3] Weizmann Inst Sci, Dept Comp Sci & Appl Math, IL-76100 Rehovot, Israel
[4] Jagiellonian Univ, Inst Comp Sci, Lojasiewicza 6, PL-30348 Krakow, Poland
[5] Rutgers State Univ, Dept Math, 110 Frelinghusen Rd, Piscataway, NJ 08854 USA
基金
美国国家科学基金会;
关键词
Navier-Stokes; Euler equations; Turbulence; Averaging; Landau damping; EQUATIONS;
D O I
10.1016/j.physd.2017.12.010
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
The paper studies the issue of stability of solutions to the forced Navier-Stokes and damped Euler systems in periodic boxes. It is shown that for large, but fixed, Grashoff (Reynolds) number the turbulent behavior of all Leray-Hopf weak solutions of the three-dimensional Navier-Stokes equations, in periodic box, is suppressed, when viewed in the right frame of reference, by large enough average flow of the initial data; a phenomenon that is similar in spirit to the Landau damping. Specifically, we consider an initial data which have large enough spatial average, then by means of the Galilean transformation, and thanks to the periodic boundary conditions, the large time independent forcing term changes into a highly oscillatory force; which then allows us to employ some averaging principles to establish our result. Moreover, we also show that under the action of fast oscillatory-in-time external forces all two-dimensional regular solutions of the Navier-Stokes and the damped Euler equations converge to a unique time-periodic solution. (C) 2017 Elsevier B.V. All rights reserved.
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页码:18 / 29
页数:12
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