<p>In this note we contribute two results to the theory of the 2<i>D</i> Euler equations in vorticity form on the full plane. First, we establish a generalized Lagrangian representation of weak (in general measure-valued) solutions, which includes and extends classical results on the Lagrangianity of weak solutions. Second, we construct nonlinear Markov processes which are uniquely determined by a selection of weak solutions from initial data in <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(L^1\cap L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>1</mn> </msup> <mo>∩</mo> <msup> <mi>L</mi> <mi>p</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(p \ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, and related spaces such as the classical and uniformly localized Yudovich space. It is well-known that for <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(p &lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> weak solutions are in general not unique, which renders a suitable selection nontrivial.</p>

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2D vorticity Euler equations: Superposition solutions and nonlinear Markov processes

  • Marco Rehmeier,
  • Marco Romito

摘要

In this note we contribute two results to the theory of the 2D Euler equations in vorticity form on the full plane. First, we establish a generalized Lagrangian representation of weak (in general measure-valued) solutions, which includes and extends classical results on the Lagrangianity of weak solutions. Second, we construct nonlinear Markov processes which are uniquely determined by a selection of weak solutions from initial data in \(L^1\cap L^p\) L 1 L p , \(p \ge 2\) p 2 , and related spaces such as the classical and uniformly localized Yudovich space. It is well-known that for \(p <\infty \) p < weak solutions are in general not unique, which renders a suitable selection nontrivial.