Cascades in helical turbulence
| dc.creator | Ditlevsen, P. D. | |
| dc.creator | Giuliani, P. | |
| dc.date | 1999-10-08 | |
| dc.date.accessioned | 2026-07-07T02:36:01Z | |
| dc.date.available | 2026-07-07T02:36:01Z | |
| dc.description | The existence of a second quadratic inviscid invariant, the helicity, in a turbulent flow leads to coexisting cascades of energy and helicity. An equivalent of the four-fifth law for the longitudinal third order structure function, which is derived from energy conservation, is easily derived from helicity conservation cite{Procaccia,russian}. The ratio of dissipation of helicity to dissipation of energy is proportional to the wave-number leading to a different Kolmogorov scale for helicity than for energy. The Kolmogorov scale for helicity is always larger than the Kolmogorov scale for energy so in the high Reynolds number limit the flow will always be helicity free in the small scales, much in the same way as the flow will be isotropic and homogeneous in the small scales. A consequence is that a pure helicity cascade is not possible. The idea is illustrated in a shell model of turbulence. | |
| dc.description | 4 pages, 4 figures | |
| dc.identifier | https://arxiv.org/abs/chao-dyn/9910013 | |
| dc.identifier | http://arxiv.org/abs/chao-dyn/9910013 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/15771 | |
| dc.subject | Chaotic Dynamics | |
| dc.title | Cascades in helical turbulence | |
| dc.type | text |