{"title":"Stabilization in two-species chemotaxis systems with singular sensitivity and Lotka-Volterra competitive kinetics","authors":"Halil ibrahim Kurt, Wenxian Shen","doi":"10.3934/dcds.2023130","DOIUrl":null,"url":null,"abstract":"The current paper is concerned with the stabilization in the following parabolic-parabolic-elliptic chemotaxis system with singular sensitivity and Lotka-Volterra competitive kinetics, $ \\begin{equation} \\begin{cases} u_t = \\Delta u-\\chi_1 \\nabla\\cdot (\\frac{u}{w} \\nabla w)+u(a_1-b_1u-c_1v) , \\quad &x\\in \\Omega\\cr v_t = \\Delta v-\\chi_2 \\nabla\\cdot (\\frac{v}{w} \\nabla w)+v(a_2-b_2v-c_2u), \\quad &x\\in \\Omega\\cr 0 = \\Delta w-\\mu w +\\nu u+ \\lambda v, \\quad &x\\in \\Omega \\cr \\frac{\\partial u}{\\partial n} = \\frac{\\partial v}{\\partial n} = \\frac{\\partial w}{\\partial n} = 0, \\quad &x\\in\\partial\\Omega, \\end{cases} \\end{equation}~~~~(1) $ where $ \\Omega \\subset \\mathbb{R}^N $ is a bounded smooth domain, and $ \\chi_i $, $ a_i $, $ b_i $, $ c_i $ ($ i = 1, 2 $) and $ \\mu, \\, \\nu, \\, \\lambda $ are positive constants. In [25], among others, we proved that for any given nonnegative initial data $ u_0, v_0\\in C^0(\\bar\\Omega) $ with $ u_0+v_0\\not \\equiv 0 $, (1) has a unique globally defined classical solution $ (u(t, x;u_0, v_0), v(t, x;u_0, v_0), w(t, x;u_0, v_0)) $ with $ u(0, x;u_0, v_0) = u_0(x) $ and $ v(0, x;u_0, v_0) = v_0(x) $ in any space dimensional setting with any positive constants $ \\chi_i, a_i, b_i, c_i $ ($ i = 1, 2 $) and $ \\mu, \\nu, \\lambda $. In this paper, we assume that the competition in (1) is weak in the sense that $ \\frac{c_1}{b_2}<\\frac{a_1}{a_2}, \\quad \\frac{c_2}{b_1}<\\frac{a_2}{a_1}. $ Then (1) has a unique positive constant solution $ (u^*, v^*, w^*) $, where $ u^* = \\frac{a_1b_2-c_1a_2}{b_1b_2-c_1c_2}, \\quad v^* = \\frac{b_1a_2-a_1c_2}{b_1b_2-c_1c_2}, \\quad w^* = \\frac{\\nu}{\\mu}u^*+\\frac{\\lambda}{\\mu} v^*. $ We obtain some explicit conditions on $ \\chi_1, \\chi_2 $ which ensure that the positive constant solution $ (u^*, v^*, w^*) $ is globally stable, that is, for any given nonnegative initial data $ u_0, v_0\\in C^0(\\bar\\Omega) $ with $ u_0\\not \\equiv 0 $ and $ v_0\\not \\equiv 0 $, $ \\lim\\limits_{t\\to\\infty}\\Big(\\|u(t, \\cdot;u_0, v_0)-u^*\\|_\\infty +\\|v(t, \\cdot;u_0, v_0)-v^*\\|_\\infty+\\|w(t, \\cdot;u_0, v_0)-w^*\\|_\\infty\\Big) = 0. $","PeriodicalId":1,"journal":{"name":"Accounts of Chemical Research","volume":null,"pages":null},"PeriodicalIF":16.4000,"publicationDate":"2023-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Accounts of Chemical Research","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.3934/dcds.2023130","RegionNum":1,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
The current paper is concerned with the stabilization in the following parabolic-parabolic-elliptic chemotaxis system with singular sensitivity and Lotka-Volterra competitive kinetics, $ \begin{equation} \begin{cases} u_t = \Delta u-\chi_1 \nabla\cdot (\frac{u}{w} \nabla w)+u(a_1-b_1u-c_1v) , \quad &x\in \Omega\cr v_t = \Delta v-\chi_2 \nabla\cdot (\frac{v}{w} \nabla w)+v(a_2-b_2v-c_2u), \quad &x\in \Omega\cr 0 = \Delta w-\mu w +\nu u+ \lambda v, \quad &x\in \Omega \cr \frac{\partial u}{\partial n} = \frac{\partial v}{\partial n} = \frac{\partial w}{\partial n} = 0, \quad &x\in\partial\Omega, \end{cases} \end{equation}~~~~(1) $ where $ \Omega \subset \mathbb{R}^N $ is a bounded smooth domain, and $ \chi_i $, $ a_i $, $ b_i $, $ c_i $ ($ i = 1, 2 $) and $ \mu, \, \nu, \, \lambda $ are positive constants. In [25], among others, we proved that for any given nonnegative initial data $ u_0, v_0\in C^0(\bar\Omega) $ with $ u_0+v_0\not \equiv 0 $, (1) has a unique globally defined classical solution $ (u(t, x;u_0, v_0), v(t, x;u_0, v_0), w(t, x;u_0, v_0)) $ with $ u(0, x;u_0, v_0) = u_0(x) $ and $ v(0, x;u_0, v_0) = v_0(x) $ in any space dimensional setting with any positive constants $ \chi_i, a_i, b_i, c_i $ ($ i = 1, 2 $) and $ \mu, \nu, \lambda $. In this paper, we assume that the competition in (1) is weak in the sense that $ \frac{c_1}{b_2}<\frac{a_1}{a_2}, \quad \frac{c_2}{b_1}<\frac{a_2}{a_1}. $ Then (1) has a unique positive constant solution $ (u^*, v^*, w^*) $, where $ u^* = \frac{a_1b_2-c_1a_2}{b_1b_2-c_1c_2}, \quad v^* = \frac{b_1a_2-a_1c_2}{b_1b_2-c_1c_2}, \quad w^* = \frac{\nu}{\mu}u^*+\frac{\lambda}{\mu} v^*. $ We obtain some explicit conditions on $ \chi_1, \chi_2 $ which ensure that the positive constant solution $ (u^*, v^*, w^*) $ is globally stable, that is, for any given nonnegative initial data $ u_0, v_0\in C^0(\bar\Omega) $ with $ u_0\not \equiv 0 $ and $ v_0\not \equiv 0 $, $ \lim\limits_{t\to\infty}\Big(\|u(t, \cdot;u_0, v_0)-u^*\|_\infty +\|v(t, \cdot;u_0, v_0)-v^*\|_\infty+\|w(t, \cdot;u_0, v_0)-w^*\|_\infty\Big) = 0. $
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