<p>We establish the existence of Lipschitz-continuous solutions to the Cauchy–Dirichlet problem for a class of evolutionary partial differential equations of the form <Equation ID="Equ73"> <EquationSource Format="TEX">\(\begin{aligned} \partial _tu-{{\,\textrm{div}\,}}_x \nabla _\xi f(\nabla u)=0 \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mi>u</mi> <mo>-</mo> <msub> <mrow> <mspace width="0.166667em" /> <mtext>div</mtext> <mspace width="0.166667em" /> </mrow> <mi>x</mi> </msub> <msub> <mi mathvariant="normal">∇</mi> <mi>ξ</mi> </msub> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>0</mn> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>in a space-time cylinder <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Omega _T=\Omega \times (0,T)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Ω</mi> <mi>T</mi> </msub> <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> </mrow> </math></EquationSource> </InlineEquation>, subject to time-dependent boundary data <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(g:\partial _{\mathcal {P}}\Omega _T\rightarrow \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>g</mi> <mo>:</mo> <msub> <mi>∂</mi> <mi mathvariant="script">P</mi> </msub> <msub> <mi mathvariant="normal">Ω</mi> <mi>T</mi> </msub> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> prescribed on the parabolic boundary. The main novelty in our analysis is a time-dependent version of the classical bounded slope condition, imposed on the boundary data <i>g</i> along the lateral boundary <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\partial \Omega \times (0,T)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <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>. More precisely, we require that, for each fixed <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(t\in [0,T)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, the graph of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(g(\cdot ,t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>g</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> over <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\partial \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation> admits supporting hyperplanes with slopes that may vary in time but remain uniformly bounded. The key to handling time-dependent data lies in constructing more flexible upper and lower barriers.</p>

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Parabolic PDEs with Dynamic Data under a Bounded Slope Condition

  • Verena Bögelein,
  • Frank Duzaar,
  • Giulia Treu

摘要

We establish the existence of Lipschitz-continuous solutions to the Cauchy–Dirichlet problem for a class of evolutionary partial differential equations of the form \(\begin{aligned} \partial _tu-{{\,\textrm{div}\,}}_x \nabla _\xi f(\nabla u)=0 \end{aligned}\) t u - div x ξ f ( u ) = 0 in a space-time cylinder \(\Omega _T=\Omega \times (0,T)\) Ω T = Ω × ( 0 , T ) , subject to time-dependent boundary data \(g:\partial _{\mathcal {P}}\Omega _T\rightarrow \mathbb {R}\) g : P Ω T R prescribed on the parabolic boundary. The main novelty in our analysis is a time-dependent version of the classical bounded slope condition, imposed on the boundary data g along the lateral boundary \(\partial \Omega \times (0,T)\) Ω × ( 0 , T ) . More precisely, we require that, for each fixed \(t\in [0,T)\) t [ 0 , T ) , the graph of \(g(\cdot ,t)\) g ( · , t ) over \(\partial \Omega \) Ω admits supporting hyperplanes with slopes that may vary in time but remain uniformly bounded. The key to handling time-dependent data lies in constructing more flexible upper and lower barriers.