Issue |
A&A
Volume 464, Number 1, March II 2007
AMBER: Instrument description and first astrophysical results
|
|
---|---|---|
Page(s) | 341 - 349 | |
Section | The Sun | |
DOI | https://doi.org/10.1051/0004-6361:20065834 | |
Published online | 19 December 2006 |
How does the shape and thickness of the tachocline affect the distribution of the toroidal magnetic fields in the solar dynamo?
Astronomy Department, Instituto de Astronomia, Geofísica e Ciências Atmosfêricas, Universidade de São Paulo, Rua do Matão 1226, São Paulo, Brazil e-mail: guerrero,dalpino@astro.iag.usp.br
Received:
15
June
2006
Accepted:
27
October
2006
Flux-dominated solar dynamo models, which have been
demonstrated to be quite successful in reproducing most of the
observed features of the large-scale solar magnetic cycle,
generally produce an inappropriate latitudinal distribution of the
toroidal magnetic fields, showing fields of large magnitude in
polar regions where the radial shear has a maximum
amplitude. Employing a kinematic solar dynamo model, here we explore
the contributions of both the radial and the latitudinal shear in
the generation of the toroidal magnetic fields by varying the shape
and the thickness of the solar tachocline. We also explore the
effects of the diffusivity profile of the convective zone.
Considering the shear term of the dynamo
equation, , we find that
the latitudinal component is always dominant over the radial
component at producing toroidal field amplification. These results are very sensitive to the adopted diffusivity
profile, specially in the inner convection zone (which is
characterized by the diffusivity
and the radius rc of
transition between a weak and a strong turbulent region). A
diagram of the toroidal field at a latitude of
versus
the diffusivity at the convection layer for different values of
the tachocline width has revealed that these fields are mainly
eliminated for tachoclines with width
(for
cm2 s-1 and
), or for
and
almost any value of
in the appropriate solar range. For
intermediate values of
-
, strong toroidal
fields should survive at high latitudes in the butterfly diagram
and those values are therefore not suitable. We have built
butterfly diagrams for both a thin and a
thick tachocline that best match the observations.
We have also found that a prolate tachocline is able to reproduce
solar-like butterfly diagrams depending on the choice of
appropriate diffusivity profiles and tachocline width range.
Key words: Sun: magnetic fields / Sun: transition region
© ESO, 2007
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