<p>In this work, we consider the following Keller–Segel–Navier–Stokes system with density-suppressed motility and nutrient consumption <Equation ID="Equ199"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{aligned} \rho _t + \textbf{u}\cdot \nabla \rho&amp;= \Delta \left( \rho \gamma (h)\right) +\rho f(n),&amp;\qquad x\in \Omega ,\, t&gt;0,\\ h_t + \textbf{u}\cdot \nabla h&amp;= \Delta h-h+\rho ,&amp;\qquad x\in \Omega ,\, t&gt;0,\\ n_t + \textbf{u}\cdot \nabla n&amp;= \Delta n-\rho f(n),&amp;\qquad x\in \Omega ,\, t&gt;0,\\ \textbf{u}_t + (\textbf{u}\cdot \nabla ) \textbf{u}&amp;= \Delta \textbf{u}+\nabla P+\rho \nabla \Phi ,&amp;\qquad x\in \Omega ,\, t&gt;0,\\ \nabla \cdot \textbf{u}&amp;=0,&amp;\qquad x\in \Omega ,\, t&gt;0 \end{aligned} \right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>ρ</mi> <mi>t</mi> </msub> <mo>+</mo> <mi mathvariant="bold">u</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>ρ</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mfenced close=")" open="("> <mi>ρ</mi> <mi>γ</mi> <mo stretchy="false">(</mo> <mi>h</mi> <mo stretchy="false">)</mo> </mfenced> <mo>+</mo> <mi>ρ</mi> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>n</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mspace width="2em" /> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="0.166667em" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <msub> <mi>h</mi> <mi>t</mi> </msub> <mo>+</mo> <mi mathvariant="bold">u</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mi>h</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi>h</mi> <mo>-</mo> <mi>h</mi> <mo>+</mo> <mi>ρ</mi> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mspace width="2em" /> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="0.166667em" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <msub> <mi>n</mi> <mi>t</mi> </msub> <mo>+</mo> <mi mathvariant="bold">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>ρ</mi> <mi>f</mi> <mo stretchy="false">(</mo> <mi>n</mi> <mo stretchy="false">)</mo> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mspace width="2em" /> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="0.166667em" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <msub> <mi mathvariant="bold">u</mi> <mi>t</mi> </msub> <mo>+</mo> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="bold">u</mi> <mo>·</mo> <mi mathvariant="normal">∇</mi> <mo stretchy="false">)</mo> </mrow> <mi mathvariant="bold">u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi mathvariant="normal">Δ</mi> <mi mathvariant="bold">u</mi> <mo>+</mo> <mi mathvariant="normal">∇</mi> <mi>P</mi> <mo>+</mo> <mi>ρ</mi> <mi mathvariant="normal">∇</mi> <mi mathvariant="normal">Φ</mi> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mspace width="2em" /> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="0.166667em" /> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mi mathvariant="bold">u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mspace width="2em" /> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="0.166667em" /> <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">\(\Omega \subset {\mathbb {R}}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> with smooth boundary under the no-flux boundary conditions for <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> </InlineEquation>, <i>h</i>, <i>n</i> and the Dirichlet boundary condition for <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\textbf{u}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="bold">u</mi> </math></EquationSource> </InlineEquation>. We showed that for general (large) regular initial data, the corresponding initial-boundary value problem possesses a global generalized solution. In particular, we proved these generalized solutions will eventually become smooth under the smallness assumption on the initial mass <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\left\| \rho (\cdot ,0)+n(\cdot ,0)\right\| _{L^{1}(\Omega )}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mfenced close="∥" open="∥"> <mi>ρ</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo>,</mo> <mn>0</mn> <mo stretchy="false">)</mo> <mo>+</mo> <mi>n</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo>,</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mfenced> <mrow> <msup> <mi>L</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> </math></EquationSource> </InlineEquation>.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Global solvability and eventual smoothness in a Keller–Segel–Navier–Stokes system with density-suppressed motility and nutrient consumption

  • Ju Zhou

摘要

In this work, we consider the following Keller–Segel–Navier–Stokes system with density-suppressed motility and nutrient consumption \(\begin{aligned} \left\{ \begin{aligned} \rho _t + \textbf{u}\cdot \nabla \rho&= \Delta \left( \rho \gamma (h)\right) +\rho f(n),&\qquad x\in \Omega ,\, t>0,\\ h_t + \textbf{u}\cdot \nabla h&= \Delta h-h+\rho ,&\qquad x\in \Omega ,\, t>0,\\ n_t + \textbf{u}\cdot \nabla n&= \Delta n-\rho f(n),&\qquad x\in \Omega ,\, t>0,\\ \textbf{u}_t + (\textbf{u}\cdot \nabla ) \textbf{u}&= \Delta \textbf{u}+\nabla P+\rho \nabla \Phi ,&\qquad x\in \Omega ,\, t>0,\\ \nabla \cdot \textbf{u}&=0,&\qquad x\in \Omega ,\, t>0 \end{aligned} \right. \end{aligned}\) ρ t + u · ρ = Δ ρ γ ( h ) + ρ f ( n ) , x Ω , t > 0 , h t + u · h = Δ h - h + ρ , x Ω , t > 0 , n t + u · n = Δ n - ρ f ( n ) , x Ω , t > 0 , u t + ( u · ) u = Δ u + P + ρ Φ , x Ω , t > 0 , · u = 0 , x Ω , t > 0 in a bounded domain \(\Omega \subset {\mathbb {R}}^2\) Ω R 2 with smooth boundary under the no-flux boundary conditions for \(\rho \) ρ , h, n and the Dirichlet boundary condition for \(\textbf{u}\) u . We showed that for general (large) regular initial data, the corresponding initial-boundary value problem possesses a global generalized solution. In particular, we proved these generalized solutions will eventually become smooth under the smallness assumption on the initial mass \(\left\| \rho (\cdot ,0)+n(\cdot ,0)\right\| _{L^{1}(\Omega )}\) ρ ( · , 0 ) + n ( · , 0 ) L 1 ( Ω ) .