A unified approach to regularity problems for the 3D Navier-Stokes and Euler equations: the use of Kolmogorov's dissipation range

TL;DR

This paper introduces a unified framework for analyzing regularity in 3D Navier-Stokes and Euler equations based on Kolmogorov's turbulence theory, providing new criteria and conditions for solution regularity.

Contribution

It develops a dissipation wavenumber approach that bridges viscous and inviscid cases, offering weaker regularity conditions and new insights into turbulence regimes.

Findings

Leray-Hopf solutions are regular if the dissipation wavenumber is in L^{5/2}

The dissipation wavenumber is in L^1 for all Leray-Hopf solutions

Solutions are regular when spatial intermittency is close to Kolmogorov's regime

Abstract

Motivated by Kolmogorov's theory of turbulence we present a unified approach to the regularity problems for the 3D Navier-Stokes and Euler equations. We introduce a dissipation wavenumber $\Lambda (t)$ that separates low modes where the Euler dynamics is predominant from the high modes where the viscous forces take over. Then using an indifferent to the viscosity technique we obtain a new regularity criterion which is weaker than every Ladyzhenskaya-Prodi-Serrin condition in the viscous case, and reduces to the Beale-Kato-Majda criterion in the inviscid case. In the viscous case we also we prove that Leray-Hopf solutions are regular provided $\Lambda \in L^{5/2}$, which improves our previous $\Lambda \in L^\infty$ condition. We also show that $\Lambda \in L^1$ for all Leray-Hopf solutions. Finally, we prove that Leray-Hopf solutions are regular when the time-averaged spatial intermittency is small, i.e., close to Kolmogorov's regime.