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A&A 442, 345-349 (2005)
DOI: 10.1051/0004-6361:20053509
Self and mutual magnetic helicities in coronal magnetic configurations
S. Régnier1, T. Amari2 and R. C. Canfield31 ESA Research and Scientific Support Department, ESTEC, Keplerlaan 1, 2201 AZ Noordwijk, The Netherlands
e-mail: sregnier@rssd.esa.int
2 Centre de Physique Théorique, École Polytechnique, 91128 Palaiseau, France
3 Montana State University, Physics Dept., 264 EPS Building, Bozeman, MT 59717, USA
(Received 24 May 2005 / Accepted 4 July 2005 )
Abstract
Together with the magnetic energy, the magnetic helicity is an
important quantity used to describe the nature of a magnetic field
configuration. In the following, we propose a new technique to
evaluate various components of the total
magnetic helicity in the corona for an equilibrium reconstructed
magnetic field. The most meaningful value of helicity is the
total relative magnetic helicity which describes the linkage of the
field lines even if the volume of interest is not bounded by a
magnetic surface. In addition if the magnetic field can be
decomposed into the sum of a closed field and a reference field
(following , Berger 1999 in Magnetic Helicity in Space and Laboratory Plasmas, ed. M. R. Brown, R. C. Canfield, & A. A. Pevtsov, 1), we can introduce
three other helicity components: the self
helicity of the closed field, the mutual helicity between the closed
field and the reference field, and the vacuum helicity (self
helicity of the reference field). To understand the meaning of those
quantities, we derive them from the potential field (reference) and
the force-free field computed with the same boundary conditions for
three different cases: a single twisted flux tube derived from the
extended Gold-Hoyle solutions, a simple magnetic configuration with
three balanced sources and a constant distribution of the force-free
parameter, and the AR 8210 magnetic field observed from 17:13 UT to
21:16 UT on May 1, 1998. We analyse the meaning
of the self and mutual helicities: the self and mutual helicities
correspond to the twist and writhe of confined flux bundles, and
the crossing of field lines in the magnetic configuration
respectively. The main result is that the
magnetic configuration of AR 8210 is dominated by the mutual
helicity and not by the self helicity (twist and writhe). Our results
also show that although not gauge invariant the vacuum helicity is
sensitive to the topological complexity of the reference field.
Key words: Sun: magnetic fields -- Sun: corona -- Sun: flares
© ESO 2005
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