<p>We consider the following chemotaxis-fluid system in a two-dimensional, open, bounded domain <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation>: <Equation ID="Equ78"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} n_t + u \cdot \nabla n &amp; = \Delta n - \chi \nabla \cdot \bigl (n c^\alpha \nabla c\bigr ) + r n - \mu n^2, \\ c_t + u \cdot \nabla c &amp; = \Delta c - c + n, \\ u_t + u \cdot \nabla u &amp; = \Delta u - \nabla P + n \nabla \phi , \\ \nabla \cdot u &amp; = 0, \\ \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msub> <mi>n</mi> <mi>t</mi> </msub> <mo>+</mo> <mi>u</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>n</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>n</mi> <mo>-</mo> <mi>χ</mi> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">(</mo> </mrow> <mi>n</mi> <msup> <mi>c</mi> <mi>α</mi> </msup> <mi mathvariant="normal">∇</mi> <mi>c</mi> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">)</mo> </mrow> <mo>+</mo> <mi>r</mi> <mi>n</mi> <mo>-</mo> <mi>μ</mi> <msup> <mi>n</mi> <mn>2</mn> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>c</mi> <mi>t</mi> </msub> <mo>+</mo> <mi>u</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>c</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>c</mi> <mo>-</mo> <mi>c</mi> <mo>+</mo> <mi>n</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>+</mo> <mi>u</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>-</mo> <mi mathvariant="normal">∇</mi> <mi>P</mi> <mo>+</mo> <mi>n</mi> <mi mathvariant="normal">∇</mi> <mi>ϕ</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(r, \mu , \alpha , \chi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>r</mi> <mo>,</mo> <mi>μ</mi> <mo>,</mo> <mi>α</mi> <mo>,</mo> <mi>χ</mi> </mrow> </math></EquationSource> </InlineEquation> are positive parameters and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\phi \in W^{1,\infty }(\Omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϕ</mi> <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>. In this paper, we show that the quadratic logistic source ensures the existence of global bounded solutions under the condition <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\alpha \in \left( 0, \frac{1}{2}\right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>∈</mo> <mfenced close=")" open="("> <mn>0</mn> <mo>,</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mfenced> </mrow> </math></EquationSource> </InlineEquation>. Our proof relies on the Moser–Trudinger inequality, a parabolic regularity result in Orlicz spaces, and a variational approach.</p>

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Application of the Moser–Trudinger inequality and parabolic regularity in Orlicz spaces to a sub-linear sensitivity chemotaxis-fluid system

  • Minh Le

摘要

We consider the following chemotaxis-fluid system in a two-dimensional, open, bounded domain \(\Omega \) Ω : \(\begin{aligned} {\left\{ \begin{array}{ll} n_t + u \cdot \nabla n & = \Delta n - \chi \nabla \cdot \bigl (n c^\alpha \nabla c\bigr ) + r n - \mu n^2, \\ c_t + u \cdot \nabla c & = \Delta c - c + n, \\ u_t + u \cdot \nabla u & = \Delta u - \nabla P + n \nabla \phi , \\ \nabla \cdot u & = 0, \\ \end{array}\right. } \end{aligned}\) n t + u · n = Δ n - χ · ( n c α c ) + r n - μ n 2 , c t + u · c = Δ c - c + n , u t + u · u = Δ u - P + n ϕ , · u = 0 , where \(r, \mu , \alpha , \chi \) r , μ , α , χ are positive parameters and \(\phi \in W^{1,\infty }(\Omega )\) ϕ W 1 , ( Ω ) . In this paper, we show that the quadratic logistic source ensures the existence of global bounded solutions under the condition \(\alpha \in \left( 0, \frac{1}{2}\right) \) α 0 , 1 2 . Our proof relies on the Moser–Trudinger inequality, a parabolic regularity result in Orlicz spaces, and a variational approach.