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

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arxiv 2301.01399 v3 pith:WH3COBYR submitted 2023-01-04 math.AP

classification math.AP
keywords omegaequationmathbbalignedbegincdoteulerglobal
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abstract

We consider the three-dimensional incompressible Euler equation \begin{equation*}\left\{\begin{aligned} &\partial_t \Omega+U \cdot \nabla \Omega+\Omega\cdot \nabla U=0 \\ &\Omega(x,0)=\Omega_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.

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  1. Nearly parallel helical vortex filaments in the three dimensional Euler equations

    math.AP 2025-02 conditional novelty 7.0 of 10

    Existence of smooth 3D Euler solutions concentrating along N nearly parallel helical vortex filaments whose rotation speed matches the Klein-Majda-Damodaran model to leading order.

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