<p>In this paper, we examine the nonlinear inhomogeneous parabolic equation, considering it as <Equation ID="Equ123"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{ll} v^{\prime }-\Delta _{1}v+\vert v\vert ^{s-1}v=f&amp; \hbox {in }\Omega \times (0,T), \\ v=0 &amp; \hbox {on }\partial \Omega \times (0,T), \\ v(x,0)=v_{0}(x) &amp; \hbox {in }\Omega , \end{array} \right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msup> <mi>v</mi> <mo>′</mo> </msup> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mn>1</mn> </msub> <mi>v</mi> <mo>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>s</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi>v</mi> <mo>=</mo> <mi>f</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="0.333333em" /> <mi mathvariant="normal">Ω</mi> <mo>×</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">)</mo> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>v</mi> <mo>=</mo> <mn>0</mn> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>on</mtext> <mspace width="0.333333em" /> <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> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>v</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi>v</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="0.333333em" /> <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">\(\Delta _{1}v:= \operatorname {div}\left( \frac{D v}{|D v|}\right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mn>1</mn> </msub> <mi>v</mi> <mo>:</mo> <mo>=</mo> <mo>div</mo> <mfenced close=")" open="("> <mfrac> <mrow> <mi mathvariant="italic">Dv</mi> </mrow> <mrow> <mo stretchy="false">|</mo> <mi>D</mi> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> </mfrac> </mfenced> </mrow> </math></EquationSource> </InlineEquation> is the 1-Laplacian operator, the set <InlineEquation ID="IEq2"> <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> is an open bounded domain with a 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> satisfying the Lipschitz condition, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\( T&gt;0,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mo>&gt;</mo> <mn>0</mn> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\( s\ge 1,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>≥</mo> <mn>1</mn> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\( v_{0}\in L^{2}(\Omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>v</mi> <mn>0</mn> </msub> <mo>∈</mo> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <i>f</i> is a member of the Lebesgue space. We demonstrate the existence and uniqueness of a solution to the problem.</p>

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Inhomogeneous parabolic equation associated with the 1-Laplace operator

  • Mohamed EL Hichami,
  • Youssef El Hadfi

摘要

In this paper, we examine the nonlinear inhomogeneous parabolic equation, considering it as \(\begin{aligned} \left\{ \begin{array}{ll} v^{\prime }-\Delta _{1}v+\vert v\vert ^{s-1}v=f& \hbox {in }\Omega \times (0,T), \\ v=0 & \hbox {on }\partial \Omega \times (0,T), \\ v(x,0)=v_{0}(x) & \hbox {in }\Omega , \end{array} \right. \end{aligned}\) v - Δ 1 v + | v | s - 1 v = f in Ω × ( 0 , T ) , v = 0 on Ω × ( 0 , T ) , v ( x , 0 ) = v 0 ( x ) in Ω , where \(\Delta _{1}v:= \operatorname {div}\left( \frac{D v}{|D v|}\right) \) Δ 1 v : = div Dv | D v | is the 1-Laplacian operator, the set \(\Omega \subset \mathbb {R}^{N}\) Ω R N is an open bounded domain with a boundary \( \partial \Omega \) Ω satisfying the Lipschitz condition, \( T>0,\) T > 0 , \( s\ge 1,\) s 1 , \( v_{0}\in L^{2}(\Omega )\) v 0 L 2 ( Ω ) and f is a member of the Lebesgue space. We demonstrate the existence and uniqueness of a solution to the problem.