<p>The primary intention of this article centers on the global existence of uniform-in-time boundedness for the chemotaxis system capturing T-cell dynamics, posed in a general bounded domain <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^{N}(N\ge 2)\)</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> <mo stretchy="false">(</mo> <mi>N</mi> <mo>≥</mo> <mn>2</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with smooth boundary <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\partial \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation>, where the parameter <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> is anticipated to be positive. It is clearly confirmed that for any choice of the nonnegative initial data <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(u_{0}\in C^{0}(\bar{\Omega })\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>u</mi> <mn>0</mn> </msub> <mo>∈</mo> <msup> <mi>C</mi> <mn>0</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mover accent="true"> <mrow> <mi mathvariant="normal">Ω</mi> </mrow> <mrow> <mo stretchy="false">¯</mo> </mrow> </mover> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(v_{0}\in W^{1,\infty }(\Omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>v</mi> <mn>0</mn> </msub> <mo>∈</mo> <msup> <mi>W</mi> <mrow> <mn>1</mn> <mo>,</mo> <mi>∞</mi> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, then the corresponding initial-boundary value problem (<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow /> <mo>∗</mo> </mrow> </math></EquationSource> </InlineEquation>) possesses a unique globally bounded classical solution in the structurally concrete sense of <Equation ID="Equ50"> <EquationSource Format="TEX">\( 0&lt;\max \left\{ \Vert v_{0}\Vert _{L^{\infty }(\Omega )},\frac{1}{\alpha }\right\} &lt;\pi \sqrt{\frac{2}{N}}, \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mn>0</mn> <mo>&lt;</mo> <mo movablelimits="true">max</mo> <mfenced close="}" open="{"> <mrow> <mo stretchy="false">‖</mo> </mrow> <msub> <mi>v</mi> <mn>0</mn> </msub> <msub> <mrow> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mi>∞</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> <mo>,</mo> <mfrac> <mn>1</mn> <mi>α</mi> </mfrac> </mfenced> <mo>&lt;</mo> <mi>π</mi> <msqrt> <mfrac> <mn>2</mn> <mi>N</mi> </mfrac> </msqrt> <mo>,</mo> </mrow> </math></EquationSource> </Equation>which evidently goes beyond the existing discovery of Tao-Winkler (European J. Appl. Math., 36(2025), 570–583), who asserted the same results under quite ambiguous conditions. Particularly, one of the most innovative aspects here is the construction of the weight function in <b>trigonometric form</b>, as opposed to the more conventionally exponential one or other types, showcasing remarkable versatility that can be effectively implemented to resolve a broad class of relevant chemotaxis-consumption systems.</p>

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Some further progress on global existence for chemotaxis system involving synchronous production and signal consumption

  • Jiashan Zheng,
  • Yuying Wang

摘要

The primary intention of this article centers on the global existence of uniform-in-time boundedness for the chemotaxis system capturing T-cell dynamics, posed in a general bounded domain \(\Omega \subset \mathbb {R}^{N}(N\ge 2)\) Ω R N ( N 2 ) with smooth boundary \(\partial \Omega \) Ω , where the parameter \(\alpha \) α is anticipated to be positive. It is clearly confirmed that for any choice of the nonnegative initial data \(u_{0}\in C^{0}(\bar{\Omega })\) u 0 C 0 ( Ω ¯ ) and \(v_{0}\in W^{1,\infty }(\Omega )\) v 0 W 1 , ( Ω ) , then the corresponding initial-boundary value problem ( \(*\) ) possesses a unique globally bounded classical solution in the structurally concrete sense of \( 0<\max \left\{ \Vert v_{0}\Vert _{L^{\infty }(\Omega )},\frac{1}{\alpha }\right\} <\pi \sqrt{\frac{2}{N}}, \) 0 < max v 0 L ( Ω ) , 1 α < π 2 N , which evidently goes beyond the existing discovery of Tao-Winkler (European J. Appl. Math., 36(2025), 570–583), who asserted the same results under quite ambiguous conditions. Particularly, one of the most innovative aspects here is the construction of the weight function in trigonometric form, as opposed to the more conventionally exponential one or other types, showcasing remarkable versatility that can be effectively implemented to resolve a broad class of relevant chemotaxis-consumption systems.