Fluid dynamics on logarithmic lattices

TL;DR

This paper introduces a novel approach to modeling fluid dynamics by defining velocity fields on logarithmic lattices, preserving key properties of the original equations and providing insights into turbulence and blowup phenomena.

Contribution

The authors propose a new class of simplified models for fluid dynamics that retain the exact form of original equations on logarithmic lattices, maintaining key symmetries and invariants.

Findings

Models exhibit properties similar to full fluid systems, including turbulence statistics.

Robust chaotic blowup scenarios observed in 3D Euler equations.

Solutions demonstrate existence, uniqueness, and development of singularities.

Abstract

Open problems in fluid dynamics, such as the existence of finite-time singularities (blowup), explanation of intermittency in developed turbulence, etc., are related to multi-scale structure and symmetries of underlying equations of motion. Significantly simplified equations of motion, called toy-models, are traditionally employed in the analysis of such complex systems. In such models, equations are modified preserving just a part of the structure believed to be important. Here we propose a different approach for constructing simplified models, in which instead of simplifying equations one introduces a simplified configuration space: velocity fields are defined on multi-dimensional logarithmic lattices with proper algebraic operations and calculus. Then, the equations of motion retain their exact original form and, therefore, naturally maintain most scaling properties, symmetries and invariants of the original systems. Classification of such models reveals a fascinating relation with renowned mathematical constants such as the golden mean and the plastic number. Using both rigorous and numerical analysis, we describe various properties of solutions in these models, from the basic concepts of existence and uniqueness to the blowup development and turbulent dynamics. In particular, we observe strong robustness of the chaotic blowup scenario in the three-dimensional incompressible Euler equations, as well as the Fourier mode statistics of developed turbulence resembling the full three-dimensional Navier-Stokes system.