<p>In this paper, we investigate the eigenvalue problem associated with a linear second-order elliptic operator, subject to the general Danckwerts boundary conditions: <Equation ID="Equ1"> <EquationNumber>0.1</EquationNumber> <MediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3022_Article_Equ1.gif" Format="GIF" Height="43" Rendition="HTML" Resolution="72" Type="Linedraw" Width="422" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{l} -D\varphi ''(x)+a\varphi '(x)+c(x)\varphi (x)=\lambda \varphi (x),\quad x\in (0,l),\\ D \varphi '(0)-a\varphi (0)=ab_u\varphi (0),\quad D\varphi '(l)-a\varphi (l)=-ab_d\varphi (l) \end{array}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi>D</mi> <msup> <mi>φ</mi> <mrow> <mo>′</mo> <mo>′</mo> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>a</mi> <msup> <mi>φ</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>c</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>φ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi>λ</mi> <mi>φ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="1em" /> <mi>x</mi> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>l</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>D</mi> <msup> <mi>φ</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mi>a</mi> <mi>φ</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi>a</mi> <msub> <mi>b</mi> <mi>u</mi> </msub> <mi>φ</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="1em" /> <mi>D</mi> <msup> <mi>φ</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>l</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mi>a</mi> <mi>φ</mi> <mrow> <mo stretchy="false">(</mo> <mi>l</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mo>-</mo> <mi>a</mi> <msub> <mi>b</mi> <mi>d</mi> </msub> <mi>φ</mi> <mrow> <mo stretchy="false">(</mo> <mi>l</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>in a bounded interval (0,&#xa0;<i>l</i>), where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3022_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="137" /> </InlineMediaObject> <EquationSource Format="TEX">\(b_u,b_d\in (-\infty ,+\infty ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>b</mi> <mi>u</mi> </msub> <mo>,</mo> <msub> <mi>b</mi> <mi>d</mi> </msub> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi>∞</mi> <mo>,</mo> <mo>+</mo> <mi>∞</mi> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3022_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="167" /> </InlineMediaObject> <EquationSource Format="TEX">\(D&gt;0,\,a\in (-\infty ,+\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>D</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> <mspace width="0.166667em" /> <mi>a</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mo>-</mo> <mi>∞</mi> <mo>,</mo> <mo>+</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. We provide a complete characterization of the asymptotic behaviors of the principal eigenvalue with respect to the parameters <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3022_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(b_u,b_d\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>b</mi> <mi>u</mi> </msub> <mo>,</mo> <msub> <mi>b</mi> <mi>d</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, as the diffusion rate <i>D</i> approaches zero or infinity, or as the advection rate <i>a</i> approaches infinity. The findings presented in this paper largely complement the existing literature, which offers partial results for a limited range of boundary condition parameters <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3022_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(b_u\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>b</mi> <mi>u</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3022_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(b_d\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>b</mi> <mi>d</mi> </msub> </math></EquationSource> </InlineEquation>.</p>

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Asymptotics of the principal eigenvalue of an elliptic operator with Danckwerts boundary conditions

  • Rui Peng,
  • Xin Xu,
  • Kexin Zhang,
  • Maolin Zhou

摘要

In this paper, we investigate the eigenvalue problem associated with a linear second-order elliptic operator, subject to the general Danckwerts boundary conditions: 0.1 \(\begin{aligned} \left\{ \begin{array}{l} -D\varphi ''(x)+a\varphi '(x)+c(x)\varphi (x)=\lambda \varphi (x),\quad x\in (0,l),\\ D \varphi '(0)-a\varphi (0)=ab_u\varphi (0),\quad D\varphi '(l)-a\varphi (l)=-ab_d\varphi (l) \end{array}\right. \end{aligned}\) - D φ ( x ) + a φ ( x ) + c ( x ) φ ( x ) = λ φ ( x ) , x ( 0 , l ) , D φ ( 0 ) - a φ ( 0 ) = a b u φ ( 0 ) , D φ ( l ) - a φ ( l ) = - a b d φ ( l ) in a bounded interval (0, l), where \(b_u,b_d\in (-\infty ,+\infty ]\) b u , b d ( - , + ] and \(D>0,\,a\in (-\infty ,+\infty )\) D > 0 , a ( - , + ) . We provide a complete characterization of the asymptotic behaviors of the principal eigenvalue with respect to the parameters \(b_u,b_d\) b u , b d , as the diffusion rate D approaches zero or infinity, or as the advection rate a approaches infinity. The findings presented in this paper largely complement the existing literature, which offers partial results for a limited range of boundary condition parameters \(b_u\) b u and \(b_d\) b d .