<p>This paper is devoted to the study of finite time blow-up for initial-boundary value problem to a class of semilinear parabolic equation under the influence of a linear memory term <Equation ID="Equ58"> <EquationSource Format="TEX">\(\begin{aligned} \displaystyle u_{t}-\Delta u+\int _{0}^{t}g(t-s)\Delta u(x,s)ds =|u|^{p-2}u,\quad \text{ in }\ \ \Omega \times (0, T), \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <msubsup> <mo>∫</mo> <mrow> <mn>0</mn> </mrow> <mi>t</mi> </msubsup> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo>-</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> <mi>d</mi> <mi>s</mi> <mo>=</mo> <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> <mo>,</mo> <mspace width="1em" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <mspace width="4pt" /> <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> </mstyle> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where parameter <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(p&gt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&gt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation> is a smooth bounded domain in <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathbb {R}^{n}, n\ge 1, T\in (0, \infty ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo>,</mo> <mi>n</mi> <mo>≥</mo> <mn>1</mn> <mo>,</mo> <mi>T</mi> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is the maximal existence time of solution. By virtue of the concavity method, variational method, an improved potential well method involving time variable <i>t</i> and some new differential inequality techniques, we obtain three finite time blow-up results for the problem under different initial energy levels and suitably assumptions on the relaxation function <i>g</i>, we also derive the upper bound estimation for the blow-up time. Regarding the hypotheses on initial data and function <i>g</i>, our findings improve several existing finite time blow-up conclusions.</p>

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Finite time blow-up for the semilinear parabolic equation with a memory term

  • Kailun Wang,
  • Guangyu Xu,
  • Hong Yi

摘要

This paper is devoted to the study of finite time blow-up for initial-boundary value problem to a class of semilinear parabolic equation under the influence of a linear memory term \(\begin{aligned} \displaystyle u_{t}-\Delta u+\int _{0}^{t}g(t-s)\Delta u(x,s)ds =|u|^{p-2}u,\quad \text{ in }\ \ \Omega \times (0, T), \end{aligned}\) u t - Δ u + 0 t g ( t - s ) Δ u ( x , s ) d s = | u | p - 2 u , in Ω × ( 0 , T ) , where parameter \(p>2\) p > 2 and \(\Omega \) Ω is a smooth bounded domain in \(\mathbb {R}^{n}, n\ge 1, T\in (0, \infty ]\) R n , n 1 , T ( 0 , ] is the maximal existence time of solution. By virtue of the concavity method, variational method, an improved potential well method involving time variable t and some new differential inequality techniques, we obtain three finite time blow-up results for the problem under different initial energy levels and suitably assumptions on the relaxation function g, we also derive the upper bound estimation for the blow-up time. Regarding the hypotheses on initial data and function g, our findings improve several existing finite time blow-up conclusions.