The Nonlocal-to-Local Limit for the Inviscid Leray-α Equations
Jule Schindler, Emil Wiedemann
TL;DR
This work analyzes the nonlocal-to-local (α→0) limit of the inviscid Leray-$α$ equations, addressing both strong convergence on $\mathbb{R}^d$ and weak convergence on bounded domains. It proves strong convergence in $H^s$ for $s> d/2+1$ and $d\in\{2,3\}$ for a broad kernel class, with explicit rates in $H^{s'}$, and it shows weak convergence to Euler solutions on bounded domains under a turbulence-inspired local scaling property, even allowing for anomalous dissipation. The results are obtained without relying on vorticity and under general regularising kernels $K^{α}$, clarifying the relationship between Leray-$α$ regularisation and the Euler dynamics. These findings have implications for understanding nonlocal regularisations in fluid dynamics and for turbulence modeling via α-regularisation approaches.
Abstract
We consider the inviscid Leray-$α$ equations - an inviscid nonlocal regularisation of the Euler equations. In the first part, we prove the convergence of strong solutions of the Leray-$α$ equations to strong solutions of the Euler equations in $H^s(\mathbb{R}^d)$ for $s>d/2 +1 $, $d\in \{2,3\}$, for a large class of regularising kernels. In the second part, we consider weak solutions on a bounded domain with a local scaling property far away from the boundary. The scaling relates to second-order structure functions from turbulence theory and does not imply regularity. Nonetheless, under these assumptions, the weak solutions converge to (possibly wild) weak solutions of Euler in $L^2$ for almost every $t$.
