<p>This paper is concerned with the two-dimensional chemotaxis-fluid model <Equation ID="Equ97"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} n_t+u\cdot \nabla n=\Delta (n\phi (v))+\mu n(1-n),\\ v_t+u\cdot \nabla v=\Delta v-nv,\\ u_t+ \kappa (u\cdot \nabla ) u=\Delta u+n\nabla \Phi -\nabla P, \quad \nabla \cdot u=0, \end{array}\right. } \end{aligned}\)</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> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mrow> <mo stretchy="false">(</mo> <mi>n</mi> <mi>ϕ</mi> <mrow> <mo stretchy="false">(</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>μ</mi> <mi>n</mi> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>-</mo> <mi>n</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>v</mi> <mi>t</mi> </msub> <mo>+</mo> <mi>u</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>v</mi> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>v</mi> <mo>-</mo> <mi>n</mi> <mi>v</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>+</mo> <mi>κ</mi> <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>n</mi> <mi mathvariant="normal">∇</mi> <mi mathvariant="normal">Φ</mi> <mo>-</mo> <mi mathvariant="normal">∇</mi> <mi>P</mi> <mo>,</mo> <mspace width="1em" /> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mi>u</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>accounting for signal-dependent motilities of microbial populations interacting with an incompressible liquid through transport and buoyancy, where the suitably smooth function <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϕ</mi> </math></EquationSource> </InlineEquation> satisfies <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\phi &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϕ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> on <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\((0,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\phi (0)=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϕ</mi> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\phi '(0)&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>ϕ</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and the parameter <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mu \ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. For all reasonably regular initial data, if <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mu =0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, the corresponding initial boundary value problem possesses global classical solutions with a smallness condition on <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\int _\Omega n_0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mo>∫</mo> <mi mathvariant="normal">Ω</mi> </msub> <msub> <mi>n</mi> <mn>0</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>; whereas if <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mu &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, this problem possesses global bounded classical solutions, which can converge toward (1,0,0) as time tends to infinity when a certain small mass is imposed on the initial data <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(v_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>v</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation>. These results extend recent results for the fluid-free system to one in a Navier-Stokes fluid environment.</p>

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Global classical solutions to a two-dimensional chemotaxis-fluid system involving signal-dependent degenerate diffusion

  • Yansheng Ma,
  • Peter Y. H. Pang,
  • Yifu Wang

摘要

This paper is concerned with the two-dimensional chemotaxis-fluid model \(\begin{aligned} {\left\{ \begin{array}{ll} n_t+u\cdot \nabla n=\Delta (n\phi (v))+\mu n(1-n),\\ v_t+u\cdot \nabla v=\Delta v-nv,\\ u_t+ \kappa (u\cdot \nabla ) u=\Delta u+n\nabla \Phi -\nabla P, \quad \nabla \cdot u=0, \end{array}\right. } \end{aligned}\) n t + u · n = Δ ( n ϕ ( v ) ) + μ n ( 1 - n ) , v t + u · v = Δ v - n v , u t + κ ( u · ) u = Δ u + n Φ - P , · u = 0 , accounting for signal-dependent motilities of microbial populations interacting with an incompressible liquid through transport and buoyancy, where the suitably smooth function \(\phi \) ϕ satisfies \(\phi >0\) ϕ > 0 on \((0,\infty )\) ( 0 , ) with \(\phi (0)=0\) ϕ ( 0 ) = 0 and \(\phi '(0)>0\) ϕ ( 0 ) > 0 , and the parameter \(\mu \ge 0\) μ 0 . For all reasonably regular initial data, if \(\mu =0\) μ = 0 , the corresponding initial boundary value problem possesses global classical solutions with a smallness condition on \(\int _\Omega n_0\) Ω n 0 ; whereas if \(\mu >0\) μ > 0 , this problem possesses global bounded classical solutions, which can converge toward (1,0,0) as time tends to infinity when a certain small mass is imposed on the initial data \(v_0\) v 0 . These results extend recent results for the fluid-free system to one in a Navier-Stokes fluid environment.