<p>This paper is concerned with the following spatiotemporal population-toxicant model with toxicant-taxis in a bounded domain <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^n(n\ge 1)\)</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>1</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with inhomogeneous Robin boundary conditions <Equation ID="Equ180"> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} u_t=d\Delta u+\chi \nabla \cdot ( u\nabla w)+u(1-u)-\sigma uw,&amp; x\in \Omega ,t&gt;0\\ w_t=\varepsilon \Delta w-\mu w-\lambda uw,&amp; x\in \Omega ,t&gt;0,\\ (d\nabla u+\chi u\nabla w)\cdot \nu =0,\ \ \nabla w\cdot \nu =\xi (h(x,t)-w), &amp; x\in \partial \Omega ,t&gt;0\\ u(x,0)=u_0(x),\ \ w(x,0)=w_0(x),&amp; x\in \Omega , \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>=</mo> <mi>d</mi> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>χ</mi> <mi mathvariant="normal">∇</mi> <mo>·</mo> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mi mathvariant="normal">∇</mi> <mi>w</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>-</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mi>σ</mi> <mi>u</mi> <mi>w</mi> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mi>w</mi> <mi>t</mi> </msub> <mo>=</mo> <mi>ε</mi> <mi mathvariant="normal">Δ</mi> <mi>w</mi> <mo>-</mo> <mi>μ</mi> <mi>w</mi> <mo>-</mo> <mi>λ</mi> <mi>u</mi> <mi>w</mi> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mo stretchy="false">(</mo> <mi>d</mi> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo>+</mo> <mi>χ</mi> <mi>u</mi> <mi mathvariant="normal">∇</mi> <mi>w</mi> <mo stretchy="false">)</mo> <mo>·</mo> <mi>ν</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mspace width="4pt" /> <mspace width="4pt" /> <mi mathvariant="normal">∇</mi> <mi>w</mi> <mo>·</mo> <mi>ν</mi> <mo>=</mo> <mi>ξ</mi> <mo stretchy="false">(</mo> <mi>h</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>-</mo> <mi>w</mi> <mo stretchy="false">)</mo> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi>u</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="4pt" /> <mspace width="4pt" /> <mi>w</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi>w</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(u=u(x,t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>=</mo> <mi>u</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(w=w(x,t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>w</mi> <mo>=</mo> <mi>w</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> denote the population density and toxicant concentration at location <i>x</i> and time <i>t</i>, respectively. Here the toxicant enters the environment through the boundary with a temporally and spatially heterogeneous ambient toxicant density <i>h</i>(<i>x</i>,&#xa0;<i>t</i>). Under suitable assumptions on <i>h</i>(<i>x</i>,&#xa0;<i>t</i>), we first establish the global existence of classical solutions in two-dimensional spaces (<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(n=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>). Moreover, we show that every solution (<i>u</i>,&#xa0;<i>w</i>) converges to (1,&#xa0;0) uniformly if <i>h</i>(<i>x</i>,&#xa0;<i>t</i>) decays to zero as <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(t \rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> with a mild rate satisfying <Equation ID="Equ181"> <EquationSource Format="TEX">\(\begin{aligned} \lim \limits _{t\rightarrow \infty }\int _t^{t+1}\Vert h(\cdot ,\tau )\Vert _{L^1(\partial \Omega )}d\tau =0. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <munder> <mo movablelimits="false">lim</mo> <mrow> <mi>t</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </munder> <msubsup> <mo>∫</mo> <mi>t</mi> <mrow> <mi>t</mi> <mo>+</mo> <mn>1</mn> </mrow> </msubsup> <msub> <mrow> <mo stretchy="false">‖</mo> <mi>h</mi> <mrow> <mo stretchy="false">(</mo> <mo>·</mo> <mo>,</mo> <mi>τ</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> <mi>d</mi> <mi>τ</mi> <mo>=</mo> <mn>0</mn> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>If <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(h(x,t)\equiv h(x)\gneqq 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>h</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>≡</mo> <mi>h</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo>≩</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(0&lt;h_0=\sup _{x\in \partial \Omega }h(x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <msub> <mi>h</mi> <mn>0</mn> </msub> <mo>=</mo> <msub> <mo movablelimits="true">sup</mo> <mrow> <mi>x</mi> <mo>∈</mo> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> </mrow> </msub> <mi>h</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, we establish the existence of non-constant positive steady states in all dimensional spaces (<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(n\ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>) under the condition <Equation ID="Equ182"> <EquationSource Format="TEX">\(0&lt;h_0&lt; h^*:=\min \Big \{\frac{1}{\sigma },\frac{d}{\chi }\Big \}.\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mn>0</mn> <mo>&lt;</mo> <msub> <mi>h</mi> <mn>0</mn> </msub> <mo>&lt;</mo> <msup> <mi>h</mi> <mo>∗</mo> </msup> <mo>:</mo> <mo>=</mo> <mo movablelimits="true">min</mo> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">{</mo> </mrow> <mfrac> <mn>1</mn> <mi>σ</mi> </mfrac> <mo>,</mo> <mfrac> <mi>d</mi> <mi>χ</mi> </mfrac> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">}</mo> </mrow> <mo>.</mo> </mrow> </math></EquationSource> </Equation>We further show that this non-constant steady state is unique and globally asymptotically stable if <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(h_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>h</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> is sufficiently small. On the other hand, we prove that the species <i>u</i> is uniformly persistent if <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\sigma &lt;1/h_0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>σ</mi> <mo>&lt;</mo> <mn>1</mn> <mo stretchy="false">/</mo> <msub> <mi>h</mi> <mn>0</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>, while the toxicant-only steady state is globally asymptotically stable if <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\sigma &gt;1/M_h\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>σ</mi> <mo>&gt;</mo> <mn>1</mn> <mo stretchy="false">/</mo> <msub> <mi>M</mi> <mi>h</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> with some constant <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(M_h&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>M</mi> <mi>h</mi> </msub> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> smaller than <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(h_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>h</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation>.</p>

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Global dynamics of the toxicant-taxis model with Robin boundary conditions

  • Hai-Yang Jin,
  • King-Yeung Lam,
  • Zhi-An Wang

摘要

This paper is concerned with the following spatiotemporal population-toxicant model with toxicant-taxis in a bounded domain \(\Omega \subset \mathbb {R}^n(n\ge 1)\) Ω R n ( n 1 ) with inhomogeneous Robin boundary conditions \(\begin{aligned} {\left\{ \begin{array}{ll} u_t=d\Delta u+\chi \nabla \cdot ( u\nabla w)+u(1-u)-\sigma uw,& x\in \Omega ,t>0\\ w_t=\varepsilon \Delta w-\mu w-\lambda uw,& x\in \Omega ,t>0,\\ (d\nabla u+\chi u\nabla w)\cdot \nu =0,\ \ \nabla w\cdot \nu =\xi (h(x,t)-w), & x\in \partial \Omega ,t>0\\ u(x,0)=u_0(x),\ \ w(x,0)=w_0(x),& x\in \Omega , \end{array}\right. } \end{aligned}\) u t = d Δ u + χ · ( u w ) + u ( 1 - u ) - σ u w , x Ω , t > 0 w t = ε Δ w - μ w - λ u w , x Ω , t > 0 , ( d u + χ u w ) · ν = 0 , w · ν = ξ ( h ( x , t ) - w ) , x Ω , t > 0 u ( x , 0 ) = u 0 ( x ) , w ( x , 0 ) = w 0 ( x ) , x Ω , where \(u=u(x,t)\) u = u ( x , t ) and \(w=w(x,t)\) w = w ( x , t ) denote the population density and toxicant concentration at location x and time t, respectively. Here the toxicant enters the environment through the boundary with a temporally and spatially heterogeneous ambient toxicant density h(xt). Under suitable assumptions on h(xt), we first establish the global existence of classical solutions in two-dimensional spaces ( \(n=2\) n = 2 ). Moreover, we show that every solution (uw) converges to (1, 0) uniformly if h(xt) decays to zero as \(t \rightarrow \infty \) t with a mild rate satisfying \(\begin{aligned} \lim \limits _{t\rightarrow \infty }\int _t^{t+1}\Vert h(\cdot ,\tau )\Vert _{L^1(\partial \Omega )}d\tau =0. \end{aligned}\) lim t t t + 1 h ( · , τ ) L 1 ( Ω ) d τ = 0 . If \(h(x,t)\equiv h(x)\gneqq 0\) h ( x , t ) h ( x ) 0 with \(0<h_0=\sup _{x\in \partial \Omega }h(x)\) 0 < h 0 = sup x Ω h ( x ) , we establish the existence of non-constant positive steady states in all dimensional spaces ( \(n\ge 1\) n 1 ) under the condition \(0<h_0< h^*:=\min \Big \{\frac{1}{\sigma },\frac{d}{\chi }\Big \}.\) 0 < h 0 < h : = min { 1 σ , d χ } . We further show that this non-constant steady state is unique and globally asymptotically stable if \(h_0\) h 0 is sufficiently small. On the other hand, we prove that the species u is uniformly persistent if \(\sigma <1/h_0\) σ < 1 / h 0 , while the toxicant-only steady state is globally asymptotically stable if \(\sigma >1/M_h\) σ > 1 / M h with some constant \(M_h>0\) M h > 0 smaller than \(h_0\) h 0 .