<p>We consider the following chemotaxis system: <Equation ID="Equ99"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2477_Article_Equ99.gif" Format="GIF" Height="43" Rendition="HTML" Resolution="72" Type="Linedraw" Width="300" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} u_{t}= \Delta u - \nabla \cdot (u\nabla f(v)), \; x \in \Omega \text {, }t&gt;0,\\ v_{t}=\Delta v - u g(v), \; x \in \Omega \text {, }t&gt;0, \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>-</mo> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mi mathvariant="normal">∇</mi> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="0.277778em" /> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mtext>,</mtext> <mspace width="0.333333em" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>v</mi> <mi>t</mi> </msub> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>v</mi> <mo>-</mo> <mi>u</mi> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="0.277778em" /> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mtext>,</mtext> <mspace width="0.333333em" /> <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 bounded smooth domain <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2477_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="117" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^{n}, n=2,3 \)</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> <mo>,</mo> <mi>n</mi> <mo>=</mo> <mn>2</mn> <mo>,</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation> with nonlinear functions <i>f</i> and <i>g</i>. We establish the existence of a global classical solution under the smallness assumption on initial data. This result generalizes the existing findings for the minimal case, where <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2477_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="TEX">\(f(s)=s\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mi>s</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="33_2025_2477_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(g(s)=s.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>g</mi> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mi>s</mi> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> We further present blow-up criteria for the system.</p>

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Global classical solutions to a chemotaxis consumption system with nonlinear sensitivity and signal consumption

  • Poonam Rani,
  • Jagmohan Tyagi

摘要

We consider the following chemotaxis system: \(\begin{aligned} {\left\{ \begin{array}{ll} u_{t}= \Delta u - \nabla \cdot (u\nabla f(v)), \; x \in \Omega \text {, }t>0,\\ v_{t}=\Delta v - u g(v), \; x \in \Omega \text {, }t>0, \end{array}\right. } \end{aligned}\) u t = Δ u - · ( u f ( v ) ) , x Ω , t > 0 , v t = Δ v - u g ( v ) , x Ω , t > 0 , under homogeneous Neumann boundary conditions in a bounded smooth domain \(\Omega \subset \mathbb {R}^{n}, n=2,3 \) Ω R n , n = 2 , 3 with nonlinear functions f and g. We establish the existence of a global classical solution under the smallness assumption on initial data. This result generalizes the existing findings for the minimal case, where \(f(s)=s\) f ( s ) = s and \(g(s)=s.\) g ( s ) = s . We further present blow-up criteria for the system.