Large Time Behavior for Weak Solutions of the 3D Globally Modified Navier-Stokes Equations

This paper is concerned with the large time behavior of the weak solutions for three-dimensional globally modified Navier-Stokes equations. With the aid of energy methods and auxiliary decay estimates together with Lp-Lq estimates of heat semigroup, we derive the optimal upper and lower decay estima...

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Main Author: Junbai Ren
Format: Article
Language:English
Published: Wiley 2014-01-01
Series:Abstract and Applied Analysis
Online Access:http://dx.doi.org/10.1155/2014/879780
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author Junbai Ren
author_facet Junbai Ren
author_sort Junbai Ren
collection DOAJ
description This paper is concerned with the large time behavior of the weak solutions for three-dimensional globally modified Navier-Stokes equations. With the aid of energy methods and auxiliary decay estimates together with Lp-Lq estimates of heat semigroup, we derive the optimal upper and lower decay estimates of the weak solutions for the globally modified Navier-Stokes equations as C1(1+t)-3/4≤uL2≤C2(1+t)-3/4,  t>1. The decay rate is optimal since it coincides with that of heat equation.
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institution Kabale University
issn 1085-3375
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series Abstract and Applied Analysis
spelling doaj-art-0fec8077e00c4d8db171467d143dcc342025-02-03T01:22:05ZengWileyAbstract and Applied Analysis1085-33751687-04092014-01-01201410.1155/2014/879780879780Large Time Behavior for Weak Solutions of the 3D Globally Modified Navier-Stokes EquationsJunbai Ren0Research Center of Applied Statistics, School of Statistics, Jiangxi University of Finance and Economics, Nanchang 330013, ChinaThis paper is concerned with the large time behavior of the weak solutions for three-dimensional globally modified Navier-Stokes equations. With the aid of energy methods and auxiliary decay estimates together with Lp-Lq estimates of heat semigroup, we derive the optimal upper and lower decay estimates of the weak solutions for the globally modified Navier-Stokes equations as C1(1+t)-3/4≤uL2≤C2(1+t)-3/4,  t>1. The decay rate is optimal since it coincides with that of heat equation.http://dx.doi.org/10.1155/2014/879780
spellingShingle Junbai Ren
Large Time Behavior for Weak Solutions of the 3D Globally Modified Navier-Stokes Equations
Abstract and Applied Analysis
title Large Time Behavior for Weak Solutions of the 3D Globally Modified Navier-Stokes Equations
title_full Large Time Behavior for Weak Solutions of the 3D Globally Modified Navier-Stokes Equations
title_fullStr Large Time Behavior for Weak Solutions of the 3D Globally Modified Navier-Stokes Equations
title_full_unstemmed Large Time Behavior for Weak Solutions of the 3D Globally Modified Navier-Stokes Equations
title_short Large Time Behavior for Weak Solutions of the 3D Globally Modified Navier-Stokes Equations
title_sort large time behavior for weak solutions of the 3d globally modified navier stokes equations
url http://dx.doi.org/10.1155/2014/879780
work_keys_str_mv AT junbairen largetimebehaviorforweaksolutionsofthe3dgloballymodifiednavierstokesequations