<p>We study the Dirichlet problem for a class of Kirchhoff-type evolution equations involving the <i>p</i>-Laplace operator <Equation ID="Equ88"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="9_2025_2877_Article_Equ88.gif" Format="GIF" Height="33" Rendition="HTML" Resolution="72" Type="Linedraw" Width="525" /> </MediaObject> <EquationSource Format="TEX">\( u_{t}-a\left( \left\| \nabla u\right\| _{L^p(\Omega )}^{p}\right) \Delta _p u=\ln \left( \Vert u\Vert _{L^2(\Omega )}^2\right) |u|^{q(x,t)-2}u,\quad (x,t)\in \Omega \times (0,T), \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>-</mo> <mi>a</mi> <mfenced close=")" open="("> <msubsup> <mfenced close="∥" open="∥"> <mi mathvariant="normal">∇</mi> <mi>u</mi> </mfenced> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> <mi>p</mi> </msubsup> </mfenced> <msub> <mi mathvariant="normal">Δ</mi> <mi>p</mi> </msub> <mi>u</mi> <mo>=</mo> <mo>ln</mo> <mfenced close=")" open="("> <msubsup> <mrow> <mo stretchy="false">‖</mo> <mi>u</mi> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> <mn>2</mn> </msubsup> </mfenced> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>,</mo> <mspace width="1em" /> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <mi mathvariant="normal">Ω</mi> <mo>×</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </math></EquationSource> </Equation>where the coefficient of the diffusion and the source terms nonlocally depend on the sought solution. We assume that the coefficient <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="9_2025_2877_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="137" /> </InlineMediaObject> <EquationSource Format="TEX">\(a:[0,\infty )\rightarrow [0,\infty ) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>:</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> <mo stretchy="false">→</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is a non-decreasing function, and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="9_2025_2877_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="TEX">\(a(s)\rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="9_2025_2877_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="TEX">\(s\rightarrow 0^+\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo stretchy="false">→</mo> <msup> <mn>0</mn> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>; therefore, the equation degenerates as <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="9_2025_2877_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="103" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Vert \nabla u(t)\Vert _{p}\rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mo stretchy="false">‖</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">‖</mo> </mrow> <mi>p</mi> </msub> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Sufficient conditions for local and global in time solvability of the problem are found. The phenomena of blow-up or vanishing of solutions in a finite time are studied, and the upper bound for the blow-up moment is found.</p>

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On a Class of Kirchhoff Type p-Laplacian Evolution Equation with Nonlocal Logarithmic Nonlinearity

  • Uğur Sert,
  • Sergey Shmarev

摘要

We study the Dirichlet problem for a class of Kirchhoff-type evolution equations involving the p-Laplace operator \( u_{t}-a\left( \left\| \nabla u\right\| _{L^p(\Omega )}^{p}\right) \Delta _p u=\ln \left( \Vert u\Vert _{L^2(\Omega )}^2\right) |u|^{q(x,t)-2}u,\quad (x,t)\in \Omega \times (0,T), \) u t - a u L p ( Ω ) p Δ p u = ln u L 2 ( Ω ) 2 | u | q ( x , t ) - 2 u , ( x , t ) Ω × ( 0 , T ) , where the coefficient of the diffusion and the source terms nonlocally depend on the sought solution. We assume that the coefficient \(a:[0,\infty )\rightarrow [0,\infty ) \) a : [ 0 , ) [ 0 , ) is a non-decreasing function, and \(a(s)\rightarrow 0\) a ( s ) 0 as \(s\rightarrow 0^+\) s 0 + ; therefore, the equation degenerates as \(\Vert \nabla u(t)\Vert _{p}\rightarrow 0\) u ( t ) p 0 . Sufficient conditions for local and global in time solvability of the problem are found. The phenomena of blow-up or vanishing of solutions in a finite time are studied, and the upper bound for the blow-up moment is found.