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关于二维Shnirelman不等式:不可逆行为与Euler-Lagrange变分公式

On Shnirelman's inequality in 2D: Irreversible behavior and Euler-Lagrange variational formulation

Stefan Schiffer, Martina Zizza

arXiv 2609.31294首次发表:更新:

发表机构

Max-Planck Institute for Mathematics in the Sciences(马克斯·普朗克科学促进学会数理研究所)

机构由 AI 辅助整理,请以论文原文为准。

AI 中文总结

本文证明二维正方形中Shnirelman不等式的一个版本,构造散度自由速度场连接目标流体构型与恒等映射,其范数由$L^p$差界定,因二维拓扑障碍允许轨迹相交,导致不可逆行为。

AI 中文摘要

本文证明了二维正方形$[0,1]^2$中Shnirelman不等式的一个版本。更精确地说,给定目标流体构型$f$(一个保体积微分同胚),我们构造一个散度自由的速度场$v\in L^q_tL^p_x$,其流将$f$连接到恒等映射,且其$L^q_{t} L^p_x$-范数可有效地由$f$与$id$的$L^p$-差界定。然而,向量场的更高正则性可能受到影响。与高维情形的主要区别在于,由于维度$\nu=2$的拓扑障碍,我们必须允许不同的流体轨迹在空间中“相交”。我们还观察到,这一选择导致了欧拉动力学中不可逆行为的出现。

英文摘要

In this paper we prove a version of Shnirelman's inequality in the two-dimensional square $[0,1]^2$. More precisely, given a target fluid configuration $f$ (a volume-preserving diffeomorphism) we construct a divergence-free velocity field $v\in L^q_tL^p_x$ whose flow connects $f$ to the identity and whose $L^q_{t} L^p_x$-norm can effectively be bounded by the $L^p$-difference of $f$ and $id$. However, higher regularity of the vector field might be affected. The main difference with the higher dimensional case is that, because of the topological obstructions of dimension $ν=2$, we have to allow that different fluid trajectories 'intersect' in space. We also observe that this choice leads to the emergence of irreversible behaviors in the Eulerian dynamics.

论文原文

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