<p>We consider the incompressible Euler equations on an analytic domain <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="205_2025_2095_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation> with a nonhomogeneous boundary condition <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="205_2025_2095_Article_IEq2.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="84" /> </InlineMediaObject> <EquationSource Format="TEX">\(u\cdot {\textsf{n}} = {\overline{u}}\cdot {\textsf{n}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>·</mo> <mi mathvariant="sans-serif">n</mi> <mo>=</mo> <mover> <mi>u</mi> <mo>¯</mo> </mover> <mo>·</mo> <mi mathvariant="sans-serif">n</mi> </mrow> </math></EquationSource> </InlineEquation> on <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="205_2025_2095_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(\partial \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="205_2025_2095_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\({\overline{u}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <mi>u</mi> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation> is a given divergence-free analytic vector field. We establish the local well-posedness for <i>u</i> in analytic spaces without any compatibility conditions in all space dimensions. We also prove the global well-posedness in the 2D case if <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="205_2025_2095_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\({\overline{u}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <mi>u</mi> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation> decays in time sufficiently fast.</p>

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The inviscid inflow-outflow problem via analyticity

  • Igor Kukavica,
  • Wojciech Ożański,
  • Marco Sammartino

摘要

We consider the incompressible Euler equations on an analytic domain \(\Omega \) Ω with a nonhomogeneous boundary condition \(u\cdot {\textsf{n}} = {\overline{u}}\cdot {\textsf{n}}\) u · n = u ¯ · n on \(\partial \Omega \) Ω , where \({\overline{u}}\) u ¯ is a given divergence-free analytic vector field. We establish the local well-posedness for u in analytic spaces without any compatibility conditions in all space dimensions. We also prove the global well-posedness in the 2D case if \({\overline{u}}\) u ¯ decays in time sufficiently fast.