<p>This paper concerns global solvability of the degenerate Keller–Segel–Navier–Stokes system with flux-dependent sensitivity and superlinear signal production, <Equation ID="Equ77"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} n_t + u \cdot \nabla n= \nabla \cdot ( n^{m-1}\nabla n - n |\nabla c |^{-\alpha } \nabla c ), &amp; x\in \Omega , \ t&gt;0,\\ c_t + u \cdot \nabla c= \Delta c - c + n^\beta , &amp; x\in \Omega , \ t&gt;0,\\ u_t + (u \cdot \nabla ) u = \Delta u + \nabla P + n \nabla \Phi , \quad \nabla \cdot u = 0, &amp; x\in \Omega , \ t&gt;0 \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msub> <mi>n</mi> <mi>t</mi> </msub> <mrow> <mo>+</mo> <mi>u</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>n</mi> <mo>=</mo> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mo stretchy="false">(</mo> </mrow> <msup> <mi>n</mi> <mrow> <mi>m</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi mathvariant="normal">∇</mi> <mi>n</mi> <mo>-</mo> <msup> <mrow> <mi>n</mi> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> <mi>c</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mi>α</mi> </mrow> </msup> <mrow> <mi mathvariant="normal">∇</mi> <mi>c</mi> <mo stretchy="false">)</mo> <mo>,</mo> </mrow> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="4pt" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <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> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>c</mi> <mo>-</mo> <mi>c</mi> <mo>+</mo> <msup> <mi>n</mi> <mi>β</mi> </msup> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="4pt" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>+</mo> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mo stretchy="false">)</mo> </mrow> <mi>u</mi> <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 mathvariant="normal">Φ</mi> <mo>,</mo> <mspace width="1em" /> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mi>u</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="4pt" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>in a bounded domain <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> with smooth boundary, where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(m\ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(0&lt;\alpha &lt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>α</mi> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\beta \ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. The main result establishes existence of global weak solutions for any suitable initial data, provided that the parameters satisfy the condition <Equation ID="Equ78"> <EquationSource Format="TEX">\(\begin{aligned} m&gt; \max \left\{ \frac{(1-\alpha )(3\beta -1)+2}{3}, \,\frac{5-\alpha }{3(1+\alpha )} \right\} . \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi>m</mi> <mo>&gt;</mo> <mo movablelimits="true">max</mo> <mfenced close="}" open="{"> <mfrac> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>-</mo> <mi>α</mi> <mo stretchy="false">)</mo> <mo stretchy="false">(</mo> <mn>3</mn> <mi>β</mi> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> <mo>+</mo> <mn>2</mn> </mrow> <mn>3</mn> </mfrac> <mo>,</mo> <mspace width="0.166667em" /> <mfrac> <mrow> <mn>5</mn> <mo>-</mo> <mi>α</mi> </mrow> <mrow> <mn>3</mn> <mo stretchy="false">(</mo> <mn>1</mn> <mo>+</mo> <mi>α</mi> <mo stretchy="false">)</mo> </mrow> </mfrac> </mfenced> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation></p>

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Global solvability of a three-dimensional degenerate Keller–Segel–Navier–Stokes system with flux-dependent sensitivity and superlinear production

  • Jiyuan Guo

摘要

This paper concerns global solvability of the degenerate Keller–Segel–Navier–Stokes system with flux-dependent sensitivity and superlinear signal production, \(\begin{aligned} {\left\{ \begin{array}{ll} n_t + u \cdot \nabla n= \nabla \cdot ( n^{m-1}\nabla n - n |\nabla c |^{-\alpha } \nabla c ), & x\in \Omega , \ t>0,\\ c_t + u \cdot \nabla c= \Delta c - c + n^\beta , & x\in \Omega , \ t>0,\\ u_t + (u \cdot \nabla ) u = \Delta u + \nabla P + n \nabla \Phi , \quad \nabla \cdot u = 0, & x\in \Omega , \ t>0 \end{array}\right. } \end{aligned}\) n t + u · n = · ( n m - 1 n - n | c | - α c ) , x Ω , t > 0 , c t + u · c = Δ c - c + n β , x Ω , t > 0 , u t + ( u · ) u = Δ u + P + n Φ , · u = 0 , x Ω , t > 0 in a bounded domain \(\Omega \subset \mathbb {R}^3\) Ω R 3 with smooth boundary, where \(m\ge 1\) m 1 , \(0<\alpha <1\) 0 < α < 1 and \(\beta \ge 1\) β 1 . The main result establishes existence of global weak solutions for any suitable initial data, provided that the parameters satisfy the condition \(\begin{aligned} m> \max \left\{ \frac{(1-\alpha )(3\beta -1)+2}{3}, \,\frac{5-\alpha }{3(1+\alpha )} \right\} . \end{aligned}\) m > max ( 1 - α ) ( 3 β - 1 ) + 2 3 , 5 - α 3 ( 1 + α ) .