1. The breakout model: an interrupted numerical experiment
The breakout scenario proposes that flares with mass
ejection occur by first opening a (special) magnetic structure at the neutral
point, and then eject the plasma (Antiochos,
Devore, Klimchuk, Astrophys.J. 510, 485). This is illustrated by a very
short FILM (mov,
0.7 Mo;
gif, 1,1
Mo) showing a time-dependent solution of the MHD equations.
The initial magnetic structure
shown has a weak (neutral) point at the top of it. This weak
point is supposed, via a shear at the basis (photosphere) to lead to the
opening of the structure, and then to the flare.
The film stops, just before the magnetic field
lines completely open, because, due to strong gradients, the plasma density
becomes too low. This stops the integration, so the question remains open...
2. Analysis of a particular case: reconstructing the
magnetic structure of the Bastille Day flare (1998)
The author has looked in detail at a given flare, that
of 14 July 1998. He has "reconstructed"
the three-dimensional (volume) structure just before the flare, extrapolating
the observed surface field. He has shown (see film below) that the structure
indeed contains a neutral, weak point, and observed a partial reconnection
of the field lines there 3 minutes before the flare, as proposed by the
breakout scenario. He also has found that the sheared region is not exactly
located below the neutral point, but shifted aside. The FILM (mov,
10 Mb; gif,
18 Mb) has three successive parts:
a) a view of the sun followed by a close view of the
flare region (the viewpoint changes but the scene is static)
b) the superposed reconstruction of the magnetic field
and of the detailed flare region (still static)
c) a time-dependent sequence of pictures showing the
real evolution of the flare as observed by TRACE
3. Continued...
The author is presently working on the true time-dependent
integration of the MHD equation (first paragraph), but taking into account
the shift between the shear and the neutral point.