<p>This work investigates a limit problem for an anisotropic <i>p</i>-Laplacian operator as <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2066_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="57" /> </InlineMediaObject> <EquationSource Format="TEX">\( p \rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> within the framework of viscosity solutions. Specifically, we analyze the asymptotic behavior of an eigenvalue problem subject to Robin and mixed boundary conditions: <Equation ID="Equ90"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2066_Article_Equ90.gif" Format="GIF" Height="54" Rendition="HTML" Resolution="72" Type="Linedraw" Width="332" /> </MediaObject> <EquationSource Format="TEX">\( \left\{ \begin{aligned} -\operatorname {div} {\mathscr {H}}_{p}(\nabla u)&amp;= \Lambda _p |u|^{p-2} u &amp; \text {in } \Omega , \\ {\mathscr {H}}_{p}(\nabla u) \cdot \nu + \beta ^p |u|^{p-2} u&amp;= {\Lambda _p |u|^{p-2} u} &amp; \text {on } \partial \Omega . \end{aligned} \right. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mo>-</mo> <mo>div</mo> <msub> <mi mathvariant="script">H</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <msub> <mi mathvariant="normal">Λ</mi> <mi>p</mi> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>in</mtext> <mspace width="0.333333em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <msub> <mi mathvariant="script">H</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>·</mo> <mi>ν</mi> <mo>+</mo> <msup> <mi>β</mi> <mi>p</mi> </msup> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mrow> <msub> <mi mathvariant="normal">Λ</mi> <mi>p</mi> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> </mrow> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>on</mtext> <mspace width="0.333333em" /> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>We demonstrate that the limit of the eigenfunction is a viscosity solution to an eigenvalue problem governed by an anisotropic <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2066_Article_IEq6.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\( \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>∞</mi> </math></EquationSource> </InlineEquation>-Laplacian, and we establish several geometric properties of the corresponding eigenvalues. Subsequently, utilizing the eigenvalues derived in the first part, we address the problem with a forcing term <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2066_Article_IEq7.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\( f \in L^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>∈</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> and a boundary condition <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2066_Article_IEq8.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="57" /> </InlineMediaObject> <EquationSource Format="TEX">\( g \in L^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>g</mi> <mo>∈</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>. Furthermore, we investigate the asymptotic behavior of the associated solutions as <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2066_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="57" /> </InlineMediaObject> <EquationSource Format="TEX">\( p \rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>: <Equation ID="Equ91"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2066_Article_Equ91.gif" Format="GIF" Height="54" Rendition="HTML" Resolution="72" Type="Linedraw" Width="273" /> </MediaObject> <EquationSource Format="TEX">\( \left\{ \begin{aligned} -\operatorname {div} {\mathscr {H}}_{p}(\nabla u)&amp;= f &amp; \text {in } \Omega , \\ {\mathscr {H}}_{p}(\nabla u) \cdot \nu + \beta ^p |v|^{p-2} v&amp;= g &amp; \text {on } \partial \Omega . \end{aligned} \right. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mo>-</mo> <mo>div</mo> <msub> <mi mathvariant="script">H</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi>f</mi> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>in</mtext> <mspace width="0.333333em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <msub> <mi mathvariant="script">H</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>·</mo> <mi>ν</mi> <mo>+</mo> <msup> <mi>β</mi> <mi>p</mi> </msup> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>v</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi>g</mi> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>on</mtext> <mspace width="0.333333em" /> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation></p>

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Anisotropic \(p-\)Laplacian-Type Problems with Mixed Boundary Conditions and their Limit as \( p \rightarrow \infty \)

  • Juan Pablo A. Apaza,
  • João Vitor da Silva

摘要

This work investigates a limit problem for an anisotropic p-Laplacian operator as \( p \rightarrow \infty \) p within the framework of viscosity solutions. Specifically, we analyze the asymptotic behavior of an eigenvalue problem subject to Robin and mixed boundary conditions: \( \left\{ \begin{aligned} -\operatorname {div} {\mathscr {H}}_{p}(\nabla u)&= \Lambda _p |u|^{p-2} u & \text {in } \Omega , \\ {\mathscr {H}}_{p}(\nabla u) \cdot \nu + \beta ^p |u|^{p-2} u&= {\Lambda _p |u|^{p-2} u} & \text {on } \partial \Omega . \end{aligned} \right. \) - div H p ( u ) = Λ p | u | p - 2 u in Ω , H p ( u ) · ν + β p | u | p - 2 u = Λ p | u | p - 2 u on Ω . We demonstrate that the limit of the eigenfunction is a viscosity solution to an eigenvalue problem governed by an anisotropic \( \infty \) -Laplacian, and we establish several geometric properties of the corresponding eigenvalues. Subsequently, utilizing the eigenvalues derived in the first part, we address the problem with a forcing term \( f \in L^\infty \) f L and a boundary condition \( g \in L^\infty \) g L . Furthermore, we investigate the asymptotic behavior of the associated solutions as \( p \rightarrow \infty \) p : \( \left\{ \begin{aligned} -\operatorname {div} {\mathscr {H}}_{p}(\nabla u)&= f & \text {in } \Omega , \\ {\mathscr {H}}_{p}(\nabla u) \cdot \nu + \beta ^p |v|^{p-2} v&= g & \text {on } \partial \Omega . \end{aligned} \right. \) - div H p ( u ) = f in Ω , H p ( u ) · ν + β p | v | p - 2 v = g on Ω .