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二维纳维-斯托克斯方程无粘极限的KAM方法。

A KAM Approach to the Inviscid Limit for the 2D Navier-Stokes Equations.

作者信息

Franzoi Luca, Montalto Riccardo

机构信息

Dipartimento di Matematica "Federigo Enriques", Università degli Studi di Milano, Via Cesare Saldini 50, 20133 Milan, Italy.

出版信息

Ann Henri Poincare. 2024;25(12):5231-5275. doi: 10.1007/s00023-023-01408-9. Epub 2024 Feb 5.

DOI:10.1007/s00023-023-01408-9
PMID:39507320
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11534963/
Abstract

In this paper, we investigate the inviscid limit for time-quasi-periodic solutions of the incompressible Navier-Stokes equations on the two-dimensional torus , with a small time-quasi-periodic external force. More precisely, we construct solutions of the forced Navier-Stokes equation, bifurcating from a given time quasi-periodic solution of the incompressible Euler equations and admitting vanishing viscosity limit to the latter, uniformly for all times and independently of the size of the external perturbation. Our proof is based on the construction of an approximate solution, up to an error of order and on a fixed point argument starting with this new approximate solution. A fundamental step is to prove the invertibility of the linearized Navier-Stokes operator at a quasi-periodic solution of the Euler equation, with smallness conditions and estimates which are uniform with respect to the viscosity parameter. To the best of our knowledge, this is the first positive result for the inviscid limit problem that is global and uniform in time and it is the first KAM result in the framework of the singular limit problems.

摘要

在本文中,我们研究二维环面上具有小时间拟周期外力的不可压缩纳维 - 斯托克斯方程的时间拟周期解的无粘极限。更确切地说,我们构造受迫纳维 - 斯托克斯方程的解,它从不可压缩欧拉方程的给定时间拟周期解分叉而来,并在所有时间上一致地且与外部扰动的大小无关地允许向后者的粘性消失极限。我们的证明基于构造一个误差为 阶的近似解,并基于从此新近似解开始的不动点论证。一个基本步骤是证明在欧拉方程的拟周期解处线性化纳维 - 斯托克斯算子的可逆性,具有关于粘性参数一致的小性条件和估计。据我们所知,这是关于无粘极限问题的第一个在时间上全局且一致的肯定结果,并且是奇异极限问题框架下的第一个KAM结果。