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A&A 469, 347-354 (2007)
DOI: 10.1051/0004-6361:20077111
Profiles of heating in turbulent coronal magnetic loops
E. Buchlin1, P. J. Cargill1, S. J. Bradshaw1, and M. Velli2, 31 Space and Atmospheric Physics Department, The Blackett Laboratory, Imperial College, London SW7 2BW, UK
e-mail: e.buchlin@imperial.ac.uk
2 Dipartimento di Astronomia e Scienza dello Spazio, Università di Firenze, Largo E. Fermi 2, 50125 Firenze, Italy
3 Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109, USA
(Received 16 January 2007 / Accepted 21 March 2007)
Abstract
Context.The location of coronal heating in magnetic loops has been the subject of
a long-lasting controversy: does it occur mostly at the loop footpoints,
at the top, is it random, or is the average profile uniform?
Aims.We try to address this question in model loops with MHD turbulence and a
profile of density and/or magnetic field along the loop.
Methods. We use the SHELL-ATM MHD turbulent heating model described in Buchlin &
Velli (2007, ApJ, 662, 701), with a static mass density stratification obtained by the
HYDRAD model (Bradshaw & Mason 2003, A&A, 401, 699). This assumes the
absence of any flow or heat conduction subsequent to the dynamic
heating.
Results.
The average profile of heating is quasi-uniform, unless there is an
expansion of the flux tube (non-uniform axial magnetic field) or the
variation of the kinetic and magnetic diffusion coefficients with
temperature is taken into account: in the first case the heating is
enhanced at footpoints, whereas in the second case it is enhanced where
the dominant diffusion coefficient is enhanced.
Conclusions.
These simulations shed light on the consequences on heating profiles of
the complex interactions between physical effects involved in a
non-uniform turbulent coronal loop.
Key words: Sun: corona -- magnetohydrodynamics (MHD) -- turbulence
© ESO 2007
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