Global dynamics in a fully parabolic chemotaxis system with logistic source

Ke  Lin; Chunlai Mu

doi:10.3934/dcds.2016018

Article Contents

2016, Volume 36, Issue 9: 5025-5046. Doi: 10.3934/dcds.2016018

This issue Previous Article Topological conjugacy for Lipschitz perturbations of non-autonomous systems Next Article Local well-posedness in the critical Besov space and persistence properties for a three-component Camassa-Holm system with N-peakon solutions

Global dynamics in a fully parabolic chemotaxis system with logistic source

Ke Lin^1, and
Chunlai Mu^1,

1.
College of Mathematics and Statistics, Chongqing University, Chongqing 401331

Received: June 30, 2015

Revised: December 31, 2015

Published: May 2017

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Abstract

In this paper, we consider a fully parabolic chemotaxis system \begin{eqnarray*}\label{1} \left\{ \begin{array}{llll} u_t=\Delta u-\chi\nabla\cdot(u\nabla v)+u-\mu u^r,\quad &x\in \Omega,\quad t>0,\\ v_t=\Delta v-v+u,\quad &x\in\Omega,\quad t>0,\\ \end{array} \right. \end{eqnarray*} with homogeneous Neumann boundary conditions in an arbitrary smooth bounded domain $\Omega\subset R^n(n=2,3)$, where $\chi>0, \mu>0$ and $r\geq 2$.
For the dimensions $n=2$ and $n=3$, we establish results on the global existence and boundedness of classical solutions to the corresponding initial-boundary problem, provided that $\chi$, $\mu$ and $r$ satisfy some explicit conditions. Apart from this, we also show that if $\frac{\mu^{\frac{1}{r-1}}}{\chi}>20$ and $r\geq 2$ and $r\in \mathbb{N}$ the solution of the system approaches the steady state $\left(\mu^{-\frac{1}{r-1}}, \mu^{-\frac{1}{r-1}}\right)$ as time tends to infinity.

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Mathematics Subject Classification: Primary: 35K35, 92C17; Secondary: 35K55, 35B35.

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