On some properties of the curl operator and their consequences for the Navier-Stokes system

TL;DR

This paper explores geometric properties of the curl operator, introducing spin-definite fields to analyze 3D incompressible flows, revealing how spin conflicts lead to singularities and influence turbulence and flow regularity.

Contribution

It introduces the concept of spin-definite fields as eigenvectors of a non-local operator, providing a new geometric framework to understand Navier-Stokes singularities and flow dynamics.

Findings

Spin-definite components untangle flow rotation directions.

Finite-time blow-up involves simultaneous explosion of spin components.

Determinants involving curl and velocity relate to flow regularity and turbulence.

Abstract

We investigate some geometric properties of the $\operatorname{curl}$ operator, based on its diagonalizationand its expression as a non-local symmetry of the pseudo-derivative $(-\Delta)^{1/2}$ among divergence-free vector fieldswith finite energy. In this context, we introduce the notion of spin-definite fields, i.e. eigenvectorsof $(-\Delta)^{-1/2}\operatorname{curl}$.The two spin-definite components of a general 3D incompressible flow untangle the right-handed motion from the left-handed one. Having observed that the non-linearity of Navier-Stokes has the structure of a cross-productand its weak (distributional) form is a determinant that involves the vorticity, the velocity and a test function,we revisit the conservation of energy and the balance of helicity in a geometrical fashion. We show that in the caseof a finite-time blow-up, both spin-definite components of the flow will explose simultaneously and with equal rates,i.e. singularities in 3D are the result of a conflict of spin, which is impossible in the poorer geometry of 2D flows.We investigate the role of the local and non-local determinants $$\int_0^T\int_{\mathbb{R}^3}\det(\operatorname{curl} u, u, (-\Delta)^{\theta} u)$$ and their spin-definite counterparts, which drive the enstrophy and, more generally, are responsible forthe regularity of the flow and the emergence of singularities or quasi-singularities.As such, they are at the core of turbulence phenomena.