<p>In this paper, we examine the blow-up approximation for the semilinear reaction-diffusion equation of the following: <Equation ID="Equ58"> <EquationSource Format="TEX">\( \left\{ \begin{array}{ll} \displaystyle u_t(x,t)=u_{xx}(x,t)+u^{p}(x,t), &amp; x\in (0,1), \ t\in (0,T^{*}), \\ \displaystyle u(0,t)=0, \ \ u(1,t)=0, &amp; t\in (0,T^*), \\ \displaystyle u(x,0)=u_{0}(x)\ge 0, &amp; x\in [0,1], \end{array} \right. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi>u</mi> <mrow> <mi mathvariant="italic">xx</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <msup> <mi>u</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mstyle> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="4pt" /> <mi>t</mi> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <msup> <mi>T</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <mrow /> <mi>u</mi> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mspace width="4pt" /> <mspace width="4pt" /> <mi>u</mi> <mo stretchy="false">(</mo> <mn>1</mn> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mstyle> </mtd> <mtd columnalign="left"> <mrow> <mi>t</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <msup> <mi>T</mi> <mo>∗</mo> </msup> <mo stretchy="false">)</mo> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mstyle displaystyle="true" scriptlevel="0"> <mrow> <mrow /> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi>u</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>≥</mo> <mn>0</mn> <mo>,</mo> </mrow> </mstyle> </mtd> <mtd columnalign="left"> <mrow> <mi>x</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(p &gt; 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. By developing an appropriate semi-discrete finite difference system and incorporating the concavity method alongside a first-order inequality technique in discrete form, we derive sufficient conditions for the finite-time blow-up of solutions and establish upper bounds for the blow-up time. Furthermore, utilizing the embedding inequality and constructing suitable auxiliary functions in discrete form, we establish a lower bound for the blow-up time within the discrete scheme. Additionally, we prove the convergence of the finite difference system and the blow-up time. Lastly, numerical experiments are presented to substantiate the accuracy of the results obtained in this paper.</p>

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Blow-up in semi-discrete reaction-diffusion equations and approximation

  • Xuhui Shen,
  • Bao-Zhu Guo,
  • Yuzhe Qin

摘要

In this paper, we examine the blow-up approximation for the semilinear reaction-diffusion equation of the following: \( \left\{ \begin{array}{ll} \displaystyle u_t(x,t)=u_{xx}(x,t)+u^{p}(x,t), & x\in (0,1), \ t\in (0,T^{*}), \\ \displaystyle u(0,t)=0, \ \ u(1,t)=0, & t\in (0,T^*), \\ \displaystyle u(x,0)=u_{0}(x)\ge 0, & x\in [0,1], \end{array} \right. \) u t ( x , t ) = u xx ( x , t ) + u p ( x , t ) , x ( 0 , 1 ) , t ( 0 , T ) , u ( 0 , t ) = 0 , u ( 1 , t ) = 0 , t ( 0 , T ) , u ( x , 0 ) = u 0 ( x ) 0 , x [ 0 , 1 ] , where \(p > 1\) p > 1 . By developing an appropriate semi-discrete finite difference system and incorporating the concavity method alongside a first-order inequality technique in discrete form, we derive sufficient conditions for the finite-time blow-up of solutions and establish upper bounds for the blow-up time. Furthermore, utilizing the embedding inequality and constructing suitable auxiliary functions in discrete form, we establish a lower bound for the blow-up time within the discrete scheme. Additionally, we prove the convergence of the finite difference system and the blow-up time. Lastly, numerical experiments are presented to substantiate the accuracy of the results obtained in this paper.