Shear-current effect in a turbulent convection with a large-scale shear
| dc.creator | Rogachevskii, I. | |
| dc.creator | Kleeorin, N. | |
| dc.date | 2007-02-24 | |
| dc.date.accessioned | 2026-07-07T10:21:51Z | |
| dc.date.available | 2026-07-07T10:21:51Z | |
| dc.description | The shear-current effect in a nonrotating homogeneous turbulent convection with a large-scale constant shear is studied. The large-scale velocity shear causes anisotropy of turbulent convection, which produces the mean electromotive force $\bec{\cal E}^{(W)} \propto {\bf W} {\bf \times} {\bf J}$ and the mean electric current along the original mean magnetic field, where ${\bf W}$ is the background mean vorticity due to the shear and ${\bf J}$ is the mean electric current. This results in a large-scale dynamo even in a nonrotating and nonhelical homogeneous sheared turbulent convection, whereby the $α$ effect vanishes. It is found that turbulent convection promotes the shear-current dynamo instability, i.e., the heat flux causes positive contribution to the shear-current effect. However, there is no dynamo action due to the shear-current effect for small hydrodynamic and magnetic Reynolds numbers even in a turbulent convection, if the spatial scaling for the turbulent correlation time is $τ(k) \propto k^{-2}$, where $k$ is the small-scale wave number. | |
| dc.description | 8 pages, Physical Review E, in press | |
| dc.identifier | https://arxiv.org/abs/astro-ph/0702659 | |
| dc.identifier | http://arxiv.org/abs/astro-ph/0702659 | |
| dc.identifier | Phys.Rev.E75:046305,2007 | |
| dc.identifier | doi:10.1103/PhysRevE.75.046305 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/175314 | |
| dc.subject | Astrophysics | |
| dc.title | Shear-current effect in a turbulent convection with a large-scale shear | |
| dc.type | text |