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Global well-posedness of weak solutions to the incompressible Euler equations with helical symmetry in $\mathbb{R}^3$

Dengjun Guo, Lifeng Zhao

Abstract

We consider the three-dimensional incompressible Euler equation \begin{equation*}\left\{\begin{aligned} &\partial_t Ω+U \cdot \nabla Ω+Ω\cdot \nabla U=0 \\ &Ω(x,0)=Ω_0(x) \end{aligned}\right. \end{equation*} in the whole space $\mathbb{R}^3$. Under the assumption that the initial velocity is helical and without swirl, we prove the global well-posedness of weak solutions in $L^1_1 \bigcap L^{\infty}_1(\mathbb{R}^3)$. The vortex transport formula is also obtained in our article.

Global well-posedness of weak solutions to the incompressible Euler equations with helical symmetry in $\mathbb{R}^3$

Abstract

We consider the three-dimensional incompressible Euler equation \begin{equation*}\left\{\begin{aligned} &\partial_t Ω+U \cdot \nabla Ω+Ω\cdot \nabla U=0 \\ &Ω(x,0)=Ω_0(x) \end{aligned}\right. \end{equation*} in the whole space . Under the assumption that the initial velocity is helical and without swirl, we prove the global well-posedness of weak solutions in . The vortex transport formula is also obtained in our article.
Paper Structure (17 sections, 32 theorems, 362 equations)

This paper contains 17 sections, 32 theorems, 362 equations.

Key Result

Theorem 1.1

The two-dimensional helical Euler equation eq 2euler is globally well-posed in $L^1_1\bigcap L^{\infty}_1(\mathbb{R}^2)$ in the sense that

Theorems & Definitions (68)

  • Theorem 1.1
  • Corollary 1.2
  • Theorem 1.3
  • Lemma 2.1
  • proof
  • Definition 2.2: helical function
  • Definition 2.3: helical vector field
  • Lemma 2.4
  • proof
  • Lemma 2.5
  • ...and 58 more