<p>This paper is devoted to the fully parabolic two-species chemotaxis-competition system with nonlocal terms <Equation ID="Equ44"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="40314_2025_3280_Article_Equ44.gif" Format="GIF" Height="116" Rendition="HTML" Resolution="72" Type="Linedraw" Width="617" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{aligned}&amp;u_t=d_1\Delta u-\chi _1\nabla \cdot (u\nabla {w})+u\left( a_0-a_1u-a_2v-a_3 \int _{\Omega } u -a_4\int _{\Omega } v \right) , &amp; x\in \Omega ,t&gt;0,\\&amp;v_t=d_2\Delta {v}-\chi _2\nabla \cdot (v\nabla {w})+v\left( b_0-b_1u-b_2v-b_3 \int _{\Omega } u -b_4\int _{\Omega } v \right) , &amp; x\in \Omega ,t&gt;0,\\&amp;w_t=d_3\Delta {w}-\lambda {w}+\kappa u+\iota v, &amp; x\in \Omega ,t&gt;0, \end{aligned}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd /> <mtd columnalign="left"> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>=</mo> <msub> <mi>d</mi> <mn>1</mn> </msub> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>-</mo> <msub> <mi>χ</mi> <mn>1</mn> </msub> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mi mathvariant="normal">∇</mi> <mi>w</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>u</mi> <mfenced close=")" open="("> <msub> <mi>a</mi> <mn>0</mn> </msub> <mo>-</mo> <msub> <mi>a</mi> <mn>1</mn> </msub> <mi>u</mi> <mo>-</mo> <msub> <mi>a</mi> <mn>2</mn> </msub> <mi>v</mi> <mo>-</mo> <msub> <mi>a</mi> <mn>3</mn> </msub> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <mi>u</mi> <mo>-</mo> <msub> <mi>a</mi> <mn>4</mn> </msub> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <mi>v</mi> </mfenced> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow /> </mtd> <mtd columnalign="left"> <mrow> <msub> <mi>v</mi> <mi>t</mi> </msub> <mo>=</mo> <msub> <mi>d</mi> <mn>2</mn> </msub> <mi mathvariant="normal">Δ</mi> <mi>v</mi> <mo>-</mo> <msub> <mi>χ</mi> <mn>2</mn> </msub> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mrow> <mo stretchy="false">(</mo> <mi>v</mi> <mi mathvariant="normal">∇</mi> <mi>w</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>v</mi> <mfenced close=")" open="("> <msub> <mi>b</mi> <mn>0</mn> </msub> <mo>-</mo> <msub> <mi>b</mi> <mn>1</mn> </msub> <mi>u</mi> <mo>-</mo> <msub> <mi>b</mi> <mn>2</mn> </msub> <mi>v</mi> <mo>-</mo> <msub> <mi>b</mi> <mn>3</mn> </msub> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <mi>u</mi> <mo>-</mo> <msub> <mi>b</mi> <mn>4</mn> </msub> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <mi>v</mi> </mfenced> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow /> </mtd> <mtd columnalign="left"> <mrow> <msub> <mi>w</mi> <mi>t</mi> </msub> <mo>=</mo> <msub> <mi>d</mi> <mn>3</mn> </msub> <mi mathvariant="normal">Δ</mi> <mi>w</mi> <mo>-</mo> <mi>λ</mi> <mi>w</mi> <mo>+</mo> <mi>κ</mi> <mi>u</mi> <mo>+</mo> <mi>ι</mi> <mi>v</mi> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>under homogeneous Neumann boundary conditions in a smoothly bounded domain <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40314_2025_3280_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega \subseteq \mathbb {R}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊆</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40314_2025_3280_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="57" /> </InlineMediaObject> <EquationSource Format="TEX">\(n=1,2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>. We prove that this problem possesses a global classical solution which is uniformly bounded under the condition <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40314_2025_3280_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="505" /> </InlineMediaObject> <EquationSource Format="TEX">\((a_1+a_3|\Omega |)&gt;0,~(b_2+b_4|\Omega |)&gt;0,~ a_4 b_3 \le (a_1+a_3|\Omega |)(b_2+b_4|\Omega |)|\Omega |^{-2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> </mrow> <msub> <mi>a</mi> <mn>1</mn> </msub> <mo>+</mo> <msub> <mi>a</mi> <mn>3</mn> </msub> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">|</mo> <mo stretchy="false">)</mo> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> <mspace width="3.33333pt" /> <mo stretchy="false">(</mo> </mrow> <msub> <mi>b</mi> <mn>2</mn> </msub> <mo>+</mo> <msub> <mi>b</mi> <mn>4</mn> </msub> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">|</mo> <mo stretchy="false">)</mo> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> <mspace width="3.33333pt" /> </mrow> <msub> <mi>a</mi> <mn>4</mn> </msub> <msub> <mi>b</mi> <mn>3</mn> </msub> <mrow> <mo>≤</mo> <mo stretchy="false">(</mo> </mrow> <msub> <mi>a</mi> <mn>1</mn> </msub> <mo>+</mo> <msub> <mi>a</mi> <mn>3</mn> </msub> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">|</mo> <mo stretchy="false">)</mo> <mo stretchy="false">(</mo> </mrow> <msub> <mi>b</mi> <mn>2</mn> </msub> <mo>+</mo> <msub> <mi>b</mi> <mn>4</mn> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">|</mo> <mo stretchy="false">)</mo> <mo stretchy="false">|</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mn>2</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> in the case <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40314_2025_3280_Article_IEq4.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(n\le 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≤</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>. We obtain the fundamental estimate on <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40314_2025_3280_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Vert u\Vert _{L^{1}(\Omega )}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">‖</mo> <mi>u</mi> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40314_2025_3280_Article_IEq6.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Vert v\Vert _{L^{1}(\Omega )}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">‖</mo> <mi>v</mi> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> </math></EquationSource> </InlineEquation> by deriving a subtle estimate for <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40314_2025_3280_Article_IEq7.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="84" /> </InlineMediaObject> <EquationSource Format="TEX">\(\int _{\Omega }(u+\rho ^2v)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>+</mo> <msup> <mi>ρ</mi> <mn>2</mn> </msup> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40314_2025_3280_Article_IEq8.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> </InlineEquation> to be suitably chosen, which extends and improves the result of Xu (<CitationRef CitationID="CR38">2020</CitationRef>).</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Boundedness in a full-parabolic type chemotaxis system with competitive kinetics and nonlocal terms

  • Wenping Du,
  • Pengyan Wang

摘要

This paper is devoted to the fully parabolic two-species chemotaxis-competition system with nonlocal terms \(\begin{aligned} \left\{ \begin{aligned}&u_t=d_1\Delta u-\chi _1\nabla \cdot (u\nabla {w})+u\left( a_0-a_1u-a_2v-a_3 \int _{\Omega } u -a_4\int _{\Omega } v \right) , & x\in \Omega ,t>0,\\&v_t=d_2\Delta {v}-\chi _2\nabla \cdot (v\nabla {w})+v\left( b_0-b_1u-b_2v-b_3 \int _{\Omega } u -b_4\int _{\Omega } v \right) , & x\in \Omega ,t>0,\\&w_t=d_3\Delta {w}-\lambda {w}+\kappa u+\iota v, & x\in \Omega ,t>0, \end{aligned}\right. \end{aligned}\) u t = d 1 Δ u - χ 1 · ( u w ) + u a 0 - a 1 u - a 2 v - a 3 Ω u - a 4 Ω v , x Ω , t > 0 , v t = d 2 Δ v - χ 2 · ( v w ) + v b 0 - b 1 u - b 2 v - b 3 Ω u - b 4 Ω v , x Ω , t > 0 , w t = d 3 Δ w - λ w + κ u + ι v , x Ω , t > 0 , under homogeneous Neumann boundary conditions in a smoothly bounded domain \(\Omega \subseteq \mathbb {R}^n\) Ω R n , \(n=1,2\) n = 1 , 2 . We prove that this problem possesses a global classical solution which is uniformly bounded under the condition \((a_1+a_3|\Omega |)>0,~(b_2+b_4|\Omega |)>0,~ a_4 b_3 \le (a_1+a_3|\Omega |)(b_2+b_4|\Omega |)|\Omega |^{-2}\) ( a 1 + a 3 | Ω | ) > 0 , ( b 2 + b 4 | Ω | ) > 0 , a 4 b 3 ( a 1 + a 3 | Ω | ) ( b 2 + b 4 | Ω | ) | Ω | - 2 in the case \(n\le 2\) n 2 . We obtain the fundamental estimate on \(\Vert u\Vert _{L^{1}(\Omega )}\) u L 1 ( Ω ) and \(\Vert v\Vert _{L^{1}(\Omega )}\) v L 1 ( Ω ) by deriving a subtle estimate for \(\int _{\Omega }(u+\rho ^2v)\) Ω ( u + ρ 2 v ) with \(\rho \) ρ to be suitably chosen, which extends and improves the result of Xu (2020).