Isolating constants of motion for the homogeneous turbulence of two and three dimensions
- 1 July 1975
- journal article
- research article
- Published by AIP Publishing in Journal of Mathematical Physics
- Vol. 16 (7) , 1367-1373
- https://doi.org/10.1063/1.522705
Abstract
For the inviscid eddy motion in a finite‐dimensioned Fourier space, it is stated that energy and enstrophy are the isolating constants of motion for the 2D homogeneous turbulence. In contrast, the 3D isotropic turbulence has energy as the only constant of motion. If we relax the reflexional invariance, however, helicity emerges as another invariant; hence energy and helicity are said to be the isolating constants of motion for the helical turbulence. Although these are the key assumptions in the construction of equilibrium distributions, they have heretofore been accepted, without proof, as a natural property of the Navier–Stokes dynamics. This paper provides the proof. We have shown here that quadratic constants of motion for the individual triad‐interactions collapse to energy–enstrophy in 2D, but to energy and helicity in 3D.Keywords
This publication has 9 references indexed in Scilit:
- The triad-interaction representation of homogeneous turbulenceJournal of Mathematical Physics, 1975
- Helical turbulence and absolute equilibriumJournal of Fluid Mechanics, 1973
- Two-dimensional vortex motion and “negative temperatures”Physics Letters A, 1972
- Stationary States of Two-Dimensional TurbulencePhysical Review Letters, 1972
- The degree of knottedness of tangled vortex linesJournal of Fluid Mechanics, 1969
- Inertial Ranges in Two-Dimensional TurbulencePhysics of Fluids, 1967
- Direct-Interaction Approximation for a System of Several Interacting Simple Shear WavesPhysics of Fluids, 1963
- Statistical Analysis Based on a Certain Multivariate Complex Gaussian Distribution (An Introduction)The Annals of Mathematical Statistics, 1963
- On some statistical properties of hydrodynamical and magneto-hydrodynamical fieldsQuarterly of Applied Mathematics, 1952