<p>In this article, we investigate the interaction between two regularizing terms in the following parabolic problem <Equation ID="Equ64"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} \dfrac{\partial u}{\partial t}-\Delta u+\dfrac{\vert \nabla u\vert ^{2}}{u^{\theta }}=\dfrac{f}{u^{\gamma }}&amp; \text{ in }\ Q, \\ u(x,t)=0&amp; \text{ on }\, \Gamma , \\ u(x,0)=u_{0}(x)&amp; \text{ in }\, \Omega , \end{array}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mstyle displaystyle="true" scriptlevel="0"> <mfrac> <mrow> <mi>∂</mi> <mi>u</mi> </mrow> <mrow> <mi>∂</mi> <mi>t</mi> </mrow> </mfrac> </mstyle> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mstyle displaystyle="true" scriptlevel="0"> <mfrac> <msup> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <msup> <mi>u</mi> <mi>θ</mi> </msup> </mfrac> </mstyle> <mo>=</mo> <mstyle displaystyle="true" scriptlevel="0"> <mfrac> <mi>f</mi> <msup> <mi>u</mi> <mi>γ</mi> </msup> </mfrac> </mstyle> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <mi>Q</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mn>0</mn> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>on</mtext> <mspace width="0.333333em" /> <mspace width="0.166667em" /> <mi mathvariant="normal">Γ</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <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> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="0.166667em" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^{N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(N\ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>) is an open bounded set with boundary <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\partial \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(Q=\Omega \times (0, T)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>Q</mi> <mo>=</mo> <mi mathvariant="normal">Ω</mi> <mo>×</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(0&lt; T &lt; +\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>T</mi> <mo>&lt;</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\Gamma =\partial \Omega \times (0, T)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Γ</mi> <mo>=</mo> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>×</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(0&lt;\theta &lt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>θ</mi> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(0&lt;\gamma \le 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>γ</mi> <mo>≤</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(f\in L^{m}(Q)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>∈</mo> <msup> <mi>L</mi> <mi>m</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi>Q</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(1\le m&lt;\frac{N}{2}+1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>≤</mo> <mi>m</mi> <mo>&lt;</mo> <mfrac> <mi>N</mi> <mn>2</mn> </mfrac> <mo>+</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(u_{0}\in L^{\infty }(\Omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>u</mi> <mn>0</mn> </msub> <mo>∈</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> such that <Equation ID="Equ65"> <EquationSource Format="TEX">\(\begin{aligned} \forall \omega \subset \subset \Omega ,~\exists d_{\omega }&gt;0:~u_{0}\ge d_{\omega }~\text{ in }~\omega . \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mo>∀</mo> <mi>ω</mi> <mo>⊂</mo> <mo>⊂</mo> <mi mathvariant="normal">Ω</mi> <mo>,</mo> <mspace width="3.33333pt" /> <mo>∃</mo> <msub> <mi>d</mi> <mi>ω</mi> </msub> <mo>&gt;</mo> <mn>0</mn> <mo>:</mo> <mspace width="3.33333pt" /> <msub> <mi>u</mi> <mn>0</mn> </msub> <mo>≥</mo> <msub> <mi>d</mi> <mi>ω</mi> </msub> <mspace width="3.33333pt" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="3.33333pt" /> <mi>ω</mi> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>The aim of the paper is to extend the results recently obtained in [<CitationRef CitationID="CR2">2</CitationRef>] for the associated singular stationary problem.</p>

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Regularizing effect of the interplay between two singular nonlinearities in some parabolic equations

  • Hocine Ayadi,
  • Rezak Souilah

摘要

In this article, we investigate the interaction between two regularizing terms in the following parabolic problem \(\begin{aligned} \left\{ \begin{array}{ll} \dfrac{\partial u}{\partial t}-\Delta u+\dfrac{\vert \nabla u\vert ^{2}}{u^{\theta }}=\dfrac{f}{u^{\gamma }}& \text{ in }\ Q, \\ u(x,t)=0& \text{ on }\, \Gamma , \\ u(x,0)=u_{0}(x)& \text{ in }\, \Omega , \end{array}\right. \end{aligned}\) u t - Δ u + | u | 2 u θ = f u γ in Q , u ( x , t ) = 0 on Γ , u ( x , 0 ) = u 0 ( x ) in Ω , where \(\Omega \subset \mathbb {R}^{N}\) Ω R N ( \(N\ge 3\) N 3 ) is an open bounded set with boundary \(\partial \Omega \) Ω , \(Q=\Omega \times (0, T)\) Q = Ω × ( 0 , T ) , \(0< T < +\infty \) 0 < T < + , \(\Gamma =\partial \Omega \times (0, T)\) Γ = Ω × ( 0 , T ) , \(0<\theta <1\) 0 < θ < 1 , \(0<\gamma \le 1\) 0 < γ 1 , \(f\in L^{m}(Q)\) f L m ( Q ) , \(1\le m<\frac{N}{2}+1\) 1 m < N 2 + 1 , and \(u_{0}\in L^{\infty }(\Omega )\) u 0 L ( Ω ) such that \(\begin{aligned} \forall \omega \subset \subset \Omega ,~\exists d_{\omega }>0:~u_{0}\ge d_{\omega }~\text{ in }~\omega . \end{aligned}\) ω Ω , d ω > 0 : u 0 d ω in ω . The aim of the paper is to extend the results recently obtained in [2] for the associated singular stationary problem.