Issue |
A&A
Volume 401, Number 2, April II 2003
|
|
---|---|---|
Page(s) | 433 - 442 | |
Section | Astrophysical processes | |
DOI | https://doi.org/10.1051/0004-6361:20030207 | |
Published online | 21 March 2003 |
Box simulations of rotating magnetoconvection
Effects of penetration and turbulent pumping
Astrophysikalisches Institut Potsdam, An der Sternwarte 16, 14482 Potsdam, Germany
Corresponding author: U. Ziegler, uziegler@aip.de
Received:
3
December
2002
Accepted:
31
January
2003
Various effects of penetration in rotating magnetoconvection
are studied
by means of three-dimensional numerical simulations employing
the code NIRVANA. A local, 2-layer model is applied dividing
the computational domain (which is a rectangular box placed
tangentially on a sphere at latitude )
in an unstable polytropic region on top
of a stable polytropic region. Different realizations of
convection are examined parameterized by Taylor numbers
and
magnetic field strengths
.
We find a rather distinctive behavior
of the penetration depth Δ on the system parameters
.
In non-rotating convection Δ is a monotonically
decreasing function of
which is due to
magnetic quenching effects.
Also, penetration is subject to rotational quenching,
i.e. Δ is reduced for increasing
rotation rate. In the intermediate
regime of
, the effects of
rotation and magnetic field on Δ do not simply
add (see Fig. [see full text]). We find, nevertheless, a very strong
reduction of the penetration depth of overshooting turbulence
by both rotation and magnetism.
Penetrative convection is closely associated with the mixing
of a passive scalar quantity advected with the flow.
In the long term, the tracer material
penetrates significantly deeper into the stable layer than
suggested by Δ which is due to the cumulative effect
of isolated, fast-moving plumes. In case of a weak magnetic field,
penetrative convection also serves to ensure a downward transport
of magnetic flux by turbulent pumping
with an average rate
measured
in units of the sound speed at the top z-boundary.
For larger magnetic fields the pumping effect is quenched
and even changes sign in the convection zone. This effect is
suggested as being due to the effect of “turbulent buoyancy” which
in density-stratified media transports a given magnetic
field upwards if it is not too strong
(Kichatinov & Rüdiger [CITE]).
Key words: convection / magnetohydrodynamics / turbulence / magnetic fields
© ESO, 2003
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