<p>This paper considers the following Keller-Segel-type fully parabolic system <Equation ID="Equ149"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{aligned}&amp;u_t=\Delta (u\phi (v))+ru-\mu u^\alpha ,&amp;x\in \Omega ,t&gt;0,\\&amp;v_t=d_v\Delta v-vw,&amp;x\in \Omega ,t&gt;0,\\&amp;w_t=d_w\Delta w-w+u,&amp;x\in \Omega ,t&gt;0, \end{aligned} \right. \end{aligned}\)</EquationSource> </Equation>under no-flux boundary conditions in a smoothly bounded domain <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^n\)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(n\ge 1\)</EquationSource> </InlineEquation>, where the parameters <i>r</i>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mu \)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(d_v\)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(d_w\)</EquationSource> </InlineEquation> are positive constants and <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\alpha &gt;1\)</EquationSource> </InlineEquation>. If the motility function enjoys <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\phi \in C^3((0,\infty ))\)</EquationSource> </InlineEquation> with <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\phi (s)&gt;0\)</EquationSource> </InlineEquation> for all <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(s&gt;0\)</EquationSource> </InlineEquation>, it is shown that the system admits a global classical solution for any appropriately regular initial value when <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\alpha &gt;\max \bigl \{\frac{n+2}{4},1\bigr \}\)</EquationSource> </InlineEquation>. Additionally, if we exclude the singular at <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(s=0\)</EquationSource> </InlineEquation>, i.e., <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\phi \in C^3([0,\infty ))\)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\phi &gt;0\)</EquationSource> </InlineEquation> on <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\([0,\infty )\)</EquationSource> </InlineEquation>, then the smooth classical solution is globally bounded when any of the following conditions are met: (i) <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(n\le 5\)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\alpha &gt;1\)</EquationSource> </InlineEquation>; (ii) <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(n\ge 6\)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(\alpha &gt;2\)</EquationSource> </InlineEquation>; (iii) <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(n\ge 6\)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(\alpha =2\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(\mu &gt;\mu _*\)</EquationSource> </InlineEquation>, where <InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(\mu _*\)</EquationSource> </InlineEquation> is a positive constant independent of <i>t</i>, and further, such bounded solution will be stable at the constant <InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(\bigl ((\frac{r}{\mu })^\frac{1}{\alpha -1}, 0, (\frac{r}{\mu })^\frac{1}{\alpha -1}\bigr )\)</EquationSource> </InlineEquation> with exponential decay rate. Finally, in the case of <InlineEquation ID="IEq24"> <EquationSource Format="TEX">\(n\ge 6\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq25"> <EquationSource Format="TEX">\(1&lt;\alpha \le 2\)</EquationSource> </InlineEquation> we also showed that the system has at least one global weak solution which will become smooth after some waiting time.</p>

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Global Solvability and Boundedness for an Indirect Absorption Keller-Segel System with Signal-Dependent Motility and Logistic Source

  • Quanyong Zhao,
  • Jinrong Wang

摘要

This paper considers the following Keller-Segel-type fully parabolic system \(\begin{aligned} \left\{ \begin{aligned}&u_t=\Delta (u\phi (v))+ru-\mu u^\alpha ,&x\in \Omega ,t>0,\\&v_t=d_v\Delta v-vw,&x\in \Omega ,t>0,\\&w_t=d_w\Delta w-w+u,&x\in \Omega ,t>0, \end{aligned} \right. \end{aligned}\) under no-flux boundary conditions in a smoothly bounded domain \(\Omega \subset \mathbb {R}^n\) , \(n\ge 1\) , where the parameters r, \(\mu \) , \(d_v\) , \(d_w\) are positive constants and \(\alpha >1\) . If the motility function enjoys \(\phi \in C^3((0,\infty ))\) with \(\phi (s)>0\) for all \(s>0\) , it is shown that the system admits a global classical solution for any appropriately regular initial value when \(\alpha >\max \bigl \{\frac{n+2}{4},1\bigr \}\) . Additionally, if we exclude the singular at \(s=0\) , i.e., \(\phi \in C^3([0,\infty ))\) , \(\phi >0\) on \([0,\infty )\) , then the smooth classical solution is globally bounded when any of the following conditions are met: (i) \(n\le 5\) , \(\alpha >1\) ; (ii) \(n\ge 6\) , \(\alpha >2\) ; (iii) \(n\ge 6\) , \(\alpha =2\) and \(\mu >\mu _*\) , where \(\mu _*\) is a positive constant independent of t, and further, such bounded solution will be stable at the constant \(\bigl ((\frac{r}{\mu })^\frac{1}{\alpha -1}, 0, (\frac{r}{\mu })^\frac{1}{\alpha -1}\bigr )\) with exponential decay rate. Finally, in the case of \(n\ge 6\) and \(1<\alpha \le 2\) we also showed that the system has at least one global weak solution which will become smooth after some waiting time.