<p>In this paper we analyze the wavefront solutions of parabolic partial differential equations of the type <Equation ID="Equ45"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="30_2024_1020_Article_Equ45.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="387" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} g(u)u_{\tau }+f(u)u_{x}=(D(u)u_{x})_{x}+\rho (u),\quad u(\tau ,x)\in [0,1] \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <msub> <mi>u</mi> <mi>τ</mi> </msub> <mo>+</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <msub> <mi>u</mi> <mi>x</mi> </msub> <mo>=</mo> <msub> <mrow> <mo stretchy="false">(</mo> <mi>D</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <msub> <mi>u</mi> <mi>x</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mi>x</mi> </msub> <mo>+</mo> <mi>ρ</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="1em" /> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>τ</mi> <mo>,</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where the reaction term <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2024_1020_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> </InlineEquation> is of monostable-type. We allow the diffusivity <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2024_1020_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(D\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>D</mi> </math></EquationSource> </InlineEquation> and the accumulation term <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2024_1020_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(g\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>g</mi> </math></EquationSource> </InlineEquation> to have a finite number of changes of sign. We provide an existence result of travelling wave solutions (t.w.s.) together with an estimate of the threshold wave speed. Finally, we classify the t.w.s. between classical and sharp ones.</p>

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Wavefront solutions for reaction–diffusion–convection models with accumulation term and aggregative movements

  • Marco Cantarini,
  • Cristina Marcelli,
  • Francesca Papalini

摘要

In this paper we analyze the wavefront solutions of parabolic partial differential equations of the type \(\begin{aligned} g(u)u_{\tau }+f(u)u_{x}=(D(u)u_{x})_{x}+\rho (u),\quad u(\tau ,x)\in [0,1] \end{aligned}\) g ( u ) u τ + f ( u ) u x = ( D ( u ) u x ) x + ρ ( u ) , u ( τ , x ) [ 0 , 1 ] where the reaction term \(\rho \) ρ is of monostable-type. We allow the diffusivity \(D\) D and the accumulation term \(g\) g to have a finite number of changes of sign. We provide an existence result of travelling wave solutions (t.w.s.) together with an estimate of the threshold wave speed. Finally, we classify the t.w.s. between classical and sharp ones.