Loading…
Pattern formation by turbulent cascades
Fully developed turbulence is a universal and scale-invariant chaotic state characterized by an energy cascade from large to small scales at which the cascade is eventually arrested by dissipation 1 – 6 . Here we show how to harness these seemingly structureless turbulent cascades to generate patter...
Saved in:
Published in: | Nature (London) 2024-03, Vol.627 (8004), p.515-521 |
---|---|
Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
Summary: | Fully developed turbulence is a universal and scale-invariant chaotic state characterized by an energy cascade from large to small scales at which the cascade is eventually arrested by dissipation
1
–
6
. Here we show how to harness these seemingly structureless turbulent cascades to generate patterns. Pattern formation entails a process of wavelength selection, which can usually be traced to the linear instability of a homogeneous state
7
. By contrast, the mechanism we propose here is fully nonlinear. It is triggered by the non-dissipative arrest of turbulent cascades: energy piles up at an intermediate scale, which is neither the system size nor the smallest scales at which energy is usually dissipated. Using a combination of theory and large-scale simulations, we show that the tunable wavelength of these cascade-induced patterns can be set by a non-dissipative transport coefficient called odd viscosity, ubiquitous in chiral fluids ranging from bioactive to quantum systems
8
–
12
. Odd viscosity, which acts as a scale-dependent Coriolis-like force, leads to a two-dimensionalization of the flow at small scales, in contrast with rotating fluids in which a two-dimensionalization occurs at large scales
4
. Apart from odd viscosity fluids, we discuss how cascade-induced patterns can arise in natural systems, including atmospheric flows
13
–
19
, stellar plasma such as the solar wind
20
–
22
, or the pulverization and coagulation of objects or droplets in which mass rather than energy cascades
23
–
25
.
Turbulent energy cascades can be arrested by non-dissipative viscosities, resulting in pattern formation at intermediate length scales. |
---|---|
ISSN: | 0028-0836 1476-4687 |
DOI: | 10.1038/s41586-024-07074-z |