Boundedness properties of very weak solutions to a fully parabolic chemotaxis-system with logistic source

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• 作者：G. Viglialoro <sup>giuseppe.viglialoro@unica.it" class="auth_mail" title="E-mail the corresponding authorsup>
• 关键词：Nonlinear parabolic systems ; Chemotaxis ; Logistic source ; Boundedness
• 刊名：Nonlinear Analysis: Real World Applications
• 出版年：2017
• 出版时间：April 2017
• 年：2017
• 卷：34
• 期：Complete
• 页码：520-535
• 全文大小：707 K

文摘

In this paper we study the chemotaxis-system defined in a convex smooth and bounded domain <span id="mmlsi2" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si2.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=d9b8aa2e84d3b676fa1f52f380e355c9" title="Click to view the MathML source">Ωspan><span class="mathContainer hidden"><span class="mathCode">ath altimg="si2.gif" overflow="scroll">Ωath>span>span>span> of <span id="mmlsi3" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si3.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=8d9616131a586987a7b7a1fa36d23816" title="Click to view the MathML source">R<sup>3sup>span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si3.gif" overflow="scroll">sup>athvariant="double-struck">R3sup>ath>span>span>span>, with <span id="mmlsi4" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si4.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=7d106e8ca160730a92ce3f3abbaeb1b6" title="Click to view the MathML source">χ>0span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si4.gif" overflow="scroll">χ>0ath>span>span>span> and endowed with homogeneous Neumann boundary conditions. The source <span id="mmlsi5" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si5.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=bfb45a44b9e720dadf9275c9de4ea201" title="Click to view the MathML source">gspan><span class="mathContainer hidden"><span class="mathCode">ath altimg="si5.gif" overflow="scroll">gath>span>span>span> behaves similarly to the logistic function and verifies <span id="mmlsi6" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si6.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=99f806d5d12fe346fe1cdd082c7124d4" title="Click to view the MathML source">g(s)≤a&minus;bs<sup>αsup>span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si6.gif" overflow="scroll">g(s)≤a&minus;bsup>sαsup>ath>span>span>span>, for <span id="mmlsi7" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si7.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=07548ccbf123895e9dedaf5e86c8bf2e" title="Click to view the MathML source">s≥0span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si7.gif" overflow="scroll">s≥0ath>span>span>span>, with <span id="mmlsi8" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si8.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=c8a5418049acc909fbd3ec4d2c719278" title="Click to view the MathML source">a≥0span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si8.gif" overflow="scroll">a≥0ath>span>span>span>, <span id="mmlsi9" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si9.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=124ddd9da767694658f8ae9ecabc7c0a" title="Click to view the MathML source">b>0span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si9.gif" overflow="scroll">b>0ath>span>span>span> and <span id="mmlsi10" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si10.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=768f44717dfd1b7c521302687370734a" title="Click to view the MathML source">α>1span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si10.gif" overflow="scroll">α>1ath>span>span>span>. In line with Viglialoro (2016), where for <span id="mmlsi11" class="mathmlsrc"><a title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si11.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=df8d322462a162e145d2084b404ce802">ass="imgLazyJSB inlineImage" height="18" width="59" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S1468121816301225-si11.gif">script>style="vertical-align:bottom" width="59" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S1468121816301225-si11.gif">script>a><span class="mathContainer hidden"><span class="mathCode">ath altimg="si11.gif" overflow="scroll">α&isin;(ac>53ac>,2)ath>span>span>span> the global existence of very weak solutions <span id="mmlsi12" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si12.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=02cbdf8dbeb63e8e3e2b953f3867c909" title="Click to view the MathML source">(u,v)span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si12.gif" overflow="scroll">(u,v)ath>span>span>span> to the system is shown for any nonnegative initial data <span id="mmlsi13" class="mathmlsrc"><a title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si13.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=0e5852bdf679fc1701418596e597a6f7">ass="imgLazyJSB inlineImage" height="15" width="153" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S1468121816301225-si13.gif">script>style="vertical-align:bottom" width="153" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S1468121816301225-si13.gif">script>a><span class="mathContainer hidden"><span class="mathCode">ath altimg="si13.gif" overflow="scroll">(sub>u0sub>,sub>v0sub>)&isin;sup>C0sup>(accent="true">Ω̄)&times;sup>C2sup>(accent="true">Ω̄)ath>span>span>span> and under zero-flux boundary condition on <span id="mmlsi14" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si14.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=a18152c972549dfe65472f47343f9172" title="Click to view the MathML source">v<sub>0sub>span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si14.gif" overflow="scroll">sub>v0sub>ath>span>span>span>, we prove that no chemotactic collapse for these solutions may present over time. More precisely, we establish that if the ratio <span id="mmlsi15" class="mathmlsrc"><a title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si15.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=01c287b32702defd0b7a61fc0df50ec1">ass="imgLazyJSB inlineImage" height="15" width="8" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S1468121816301225-si15.gif">script>style="vertical-align:bottom" width="8" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S1468121816301225-si15.gif">script>a><span class="mathContainer hidden"><span class="mathCode">ath altimg="si15.gif" overflow="scroll">ac>abac>ath>span>span>span> does not exceed a certain value and for <span id="mmlsi16" class="mathmlsrc"><a title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si16.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=26c17d77bf05bbd049fb9f2b37691502">ass="imgLazyJSB inlineImage" height="17" width="89" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S1468121816301225-si16.gif">script>style="vertical-align:bottom" width="89" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S1468121816301225-si16.gif">script>a><span class="mathContainer hidden"><span class="mathCode">ath altimg="si16.gif" overflow="scroll">ac>95ac><p<α<2ath>span>span>span> the initial data are such that <span id="mmlsi17" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si17.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=28faa0bfc00b53884d83624a329342d4" title="Click to view the MathML source">‖u<sub>0sub>‖<sub>L<sup>psup>(Ω)sub>span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si17.gif" overflow="scroll">sub>‖sub>u0sub>‖sup>Lpsup>(Ω)sub>ath>span>span>span> and <span id="mmlsi18" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si18.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=14e3e9e487fd9a712c0ac38223e97025" title="Click to view the MathML source">‖&nabla;v<sub>0sub>‖<sub>L<sup>4sup>(Ω)sub>span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si18.gif" overflow="scroll">sub>‖&nabla;sub>v0sub>‖sup>L4sup>(Ω)sub>ath>span>span>span> are small enough, then <span id="mmlsi12" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S1468121816301225&_mathId=si12.gif&_user=111111111&_pii=S1468121816301225&_rdoc=1&_issn=14681218&md5=02cbdf8dbeb63e8e3e2b953f3867c909" title="Click to view the MathML source">(u,v)span><span class="mathContainer hidden"><span class="mathCode">ath altimg="si12.gif" overflow="scroll">(u,v)ath>span>span>span> is uniformly-in-time bounded.