Issue |
A&A
Volume 406, Number 1, July IV 2003
|
|
---|---|---|
Page(s) | 15 - 21 | |
Section | Astrophysical processes | |
DOI | https://doi.org/10.1051/0004-6361:20030738 | |
Published online | 17 November 2003 |
Do spherical
-dynamos oscillate?
1
Astrophysikalisches Institut Potsdam, An der Sternwarte 16, 14482 Potsdam, Germany
2
Kiepenheuer-Institut für Sonnenphysik, Schöneckstr. 6, 79104 Freiburg, Germany
Corresponding author: G. Rüdiger, gruediger@aip.de
Received:
9
December
2002
Accepted:
18
April
2003
The question of whether
kinematic -shell-dynamos are able to produce a cyclic activity
is addressed. The
α-effect is allowed to be latitudinally inhomogeneous and
anisotropic but it is assumed as radially uniform in the turbulent shell.
For a symmetric α-tensor we only find oscillatory solutions if
i) the α-tensor component
vanishes or is of the opposite sign as
, ii) the α-effect is strongly
concentrated in the equatorial region
and iii) the α-effect is
concentrated in a rather thin outer shell. In the other cases almost always the
nonaxisymmetric field mode S1 (which
slowly drifts along the azimuthal direction) possesses the lowest critical
dynamo number.
The uniform but
anisotropic α-effect (e.g.
)
leads to nonaxisymmetric solutions as is experimentally confirmed
by the Karlsruhe dynamo installation.
One of the antisymmetric parts of the
α-tensor, however, plays the role of
differential rotation in the induction equation. Using
the results of a
numerical simulation for the α-tensor of the solar convection zone for the radial
profile of this effect, one
finds the possibility of oscillating
-dynamos even without
the existence of a real nonuniform rotation law. Compared with the results
of numerical simulations of the full α-tensor, the amplitude of the
antisymmetric part of the tensor must be artifically increased by only a factor
of three in order to find oscillating solutions.
Key words: magnetohydrodynamics (MHD) / turbulence / stars: activity / earth
© ESO, 2003
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