{"title":"具有奇异敏感性和非局部项的趋化模型中的全局存在性和有界性","authors":"Wenping Du, Suying Liu, Wenji Zhang","doi":"10.1007/s00033-024-02302-y","DOIUrl":null,"url":null,"abstract":"<p>The chemotaxis system </p><span>$$\\begin{aligned} \\left\\{ \\begin{aligned}&u_t=\\Delta u-\\chi \\nabla \\cdot \\left( \\frac{u}{v}\\nabla v\\right) + u^{\\alpha }\\left( \\gamma -\\mu \\int \\limits _{\\Omega }u^{\\beta }\\right) ,{} & {} x\\in \\Omega ,t>0,\\\\&v_t=\\epsilon \\Delta v-v+u,{} & {} x\\in \\Omega ,t>0, \\end{aligned}\\right. \\end{aligned}$$</span><p>is considered under homogeneous Neumann boundary conditions in smoothly bounded domain <span>\\(\\Omega \\subseteq \\mathbb {R}^n\\)</span>, <span>\\(n\\ge 2\\)</span>, with constants <span>\\(0<\\epsilon <1\\)</span>, <span>\\(0<\\chi <1-\\epsilon \\)</span>. It is asserted that the problem possesses a uniquely global classical solution whenever the numbers <span>\\(\\alpha , \\beta \\)</span> satisfy <span>\\(1<\\alpha <2\\)</span>, <span>\\(\\beta >\\frac{n}{2}+\\alpha -1\\)</span> or <span>\\(\\alpha \\ge 2\\)</span>, <span>\\(\\beta >\\frac{n}{2}(\\alpha -1)+1\\)</span>. Moreover, it is shown that if <span>\\(1<\\alpha <2\\)</span>, <span>\\(\\beta >\\max \\{\\frac{n}{2}+\\alpha -1, \\frac{(\\alpha -1)(1-\\epsilon )}{(2-\\alpha )\\chi }+1\\}\\)</span> and <span>\\(\\gamma >0\\)</span> is sufficiently large, then the global-in-time solution is uniformly bounded. In addition, we get similar results for the case of <span>\\(n=1\\)</span>, which is worth mentioning that the requirement for <span>\\(\\epsilon \\)</span> and <span>\\(\\chi \\)</span> is very weak in the global existence result.</p>","PeriodicalId":501481,"journal":{"name":"Zeitschrift für angewandte Mathematik und Physik","volume":"14 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Global existence and boundedness in a chemotaxis model with singular sensitivity and nonlocal term\",\"authors\":\"Wenping Du, Suying Liu, Wenji Zhang\",\"doi\":\"10.1007/s00033-024-02302-y\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>The chemotaxis system </p><span>$$\\\\begin{aligned} \\\\left\\\\{ \\\\begin{aligned}&u_t=\\\\Delta u-\\\\chi \\\\nabla \\\\cdot \\\\left( \\\\frac{u}{v}\\\\nabla v\\\\right) + u^{\\\\alpha }\\\\left( \\\\gamma -\\\\mu \\\\int \\\\limits _{\\\\Omega }u^{\\\\beta }\\\\right) ,{} & {} x\\\\in \\\\Omega ,t>0,\\\\\\\\&v_t=\\\\epsilon \\\\Delta v-v+u,{} & {} x\\\\in \\\\Omega ,t>0, \\\\end{aligned}\\\\right. \\\\end{aligned}$$</span><p>is considered under homogeneous Neumann boundary conditions in smoothly bounded domain <span>\\\\(\\\\Omega \\\\subseteq \\\\mathbb {R}^n\\\\)</span>, <span>\\\\(n\\\\ge 2\\\\)</span>, with constants <span>\\\\(0<\\\\epsilon <1\\\\)</span>, <span>\\\\(0<\\\\chi <1-\\\\epsilon \\\\)</span>. It is asserted that the problem possesses a uniquely global classical solution whenever the numbers <span>\\\\(\\\\alpha , \\\\beta \\\\)</span> satisfy <span>\\\\(1<\\\\alpha <2\\\\)</span>, <span>\\\\(\\\\beta >\\\\frac{n}{2}+\\\\alpha -1\\\\)</span> or <span>\\\\(\\\\alpha \\\\ge 2\\\\)</span>, <span>\\\\(\\\\beta >\\\\frac{n}{2}(\\\\alpha -1)+1\\\\)</span>. Moreover, it is shown that if <span>\\\\(1<\\\\alpha <2\\\\)</span>, <span>\\\\(\\\\beta >\\\\max \\\\{\\\\frac{n}{2}+\\\\alpha -1, \\\\frac{(\\\\alpha -1)(1-\\\\epsilon )}{(2-\\\\alpha )\\\\chi }+1\\\\}\\\\)</span> and <span>\\\\(\\\\gamma >0\\\\)</span> is sufficiently large, then the global-in-time solution is uniformly bounded. In addition, we get similar results for the case of <span>\\\\(n=1\\\\)</span>, which is worth mentioning that the requirement for <span>\\\\(\\\\epsilon \\\\)</span> and <span>\\\\(\\\\chi \\\\)</span> is very weak in the global existence result.</p>\",\"PeriodicalId\":501481,\"journal\":{\"name\":\"Zeitschrift für angewandte Mathematik und Physik\",\"volume\":\"14 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-08-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Zeitschrift für angewandte Mathematik und Physik\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1007/s00033-024-02302-y\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Zeitschrift für angewandte Mathematik und Physik","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1007/s00033-024-02302-y","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
is considered under homogeneous Neumann boundary conditions in smoothly bounded domain \(\Omega \subseteq \mathbb {R}^n\), \(n\ge 2\), with constants \(0<\epsilon <1\), \(0<\chi <1-\epsilon \). It is asserted that the problem possesses a uniquely global classical solution whenever the numbers \(\alpha , \beta \) satisfy \(1<\alpha <2\), \(\beta >\frac{n}{2}+\alpha -1\) or \(\alpha \ge 2\), \(\beta >\frac{n}{2}(\alpha -1)+1\). Moreover, it is shown that if \(1<\alpha <2\), \(\beta >\max \{\frac{n}{2}+\alpha -1, \frac{(\alpha -1)(1-\epsilon )}{(2-\alpha )\chi }+1\}\) and \(\gamma >0\) is sufficiently large, then the global-in-time solution is uniformly bounded. In addition, we get similar results for the case of \(n=1\), which is worth mentioning that the requirement for \(\epsilon \) and \(\chi \) is very weak in the global existence result.