Issue |
A&A
Volume 421, Number 1, July I 2004
|
|
---|---|---|
Page(s) | 323 - 338 | |
Section | The Sun | |
DOI | https://doi.org/10.1051/0004-6361:20034199 | |
Published online | 11 June 2004 |
Determination of the 3D structure of an EUV-filament observed by SoHO/CDS, SoHO/SUMER and VTT/MSDP
1
Astronomical Institute, Academy of Sciences of the Czech Republic, 25165 Ondřejov, Czech Republic e-mail: pheinzel@asu.cas.cz
2
Max-Planck-Institut für Astrophysik, Karl-Schwarzschild-Strasse 1, 85740 Garching, Germany e-mail: ula@mpa-garching.mpg.de
3
Observatoire de Paris, Section Meudon, LESIA, 92195 Meudon Principal Cedex, France e-mail: brigitte.schmieder@obspm.fr
4
Institute of Theoretical Astrophysics, University of Oslo, Blindern, 0315 Oslo, Norway
Corresponding author: P. Schwartz, schwartz@asu.cas.cz
Received:
15
August
2003
Accepted:
14
February
2004
Heinzel et al. ([CITE]) found that
filaments seem to be much more extended in EUV spectral lines
than in .
In this paper we reconstruct the 3D structure of the extensions of
the EUV-filament observed
on 15 October 1999
by SoHO/CDS and SoHO/SUMER.
Small
structures were observed by VTT/MSDP.
We computed the bottom and top heights
of the EUV-filament extensions
for several values of the hydrogen
Lyman-continuum optical thickness
using
the spectroscopic model of Heinzel et al. ([CITE]).
For this we used CDS observations of the two coronal lines
624.94 Å and
520.60 Å.
Further, we develop a new method for estimating
using the
line measured by CDS and the
measured by SUMER onboard SoHO. The latter line is used as
a proxy to deduce the intensity variations of
underneath the filament.
This method also takes into
account the presence of
prominence-corona transition regions.
Resulting heights
of the EUV-filament extensions
are around 15 000 km for the bottom and around 40 000 km
for the top boundaries.
However, there are significant variations around these
representative values and we show that in about half of observed
pixels the Lyman-continuum absorption
dominates in the coronal-line depression,
while in the other half it is the volume blocking effect. The latter
situation corresponds to a large (larger than 30 000 km)
geometrical thickness of
the EUV-filament extension.
From the heights of the
boundaries of the EUV-filament
the geometrical thickness
can be computed and used to estimate the total mass
loading which was found to be comparable
to that of typical CMEs.
Key words: Sun: filaments / radiative transfer / techniques: spectroscopic / methods: data analysis
© ESO, 2004
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