Coronal heating by selective decay of MHD turbulence

Solar Physics ◽  
1988 ◽  
Vol 116 (1) ◽  
Author(s):  
D. G�mez ◽  
C.Ferro Font�n
2007 ◽  
Vol 657 (1) ◽  
pp. L47-L51 ◽  
Author(s):  
A. F. Rappazzo ◽  
M. Velli ◽  
G. Einaudi ◽  
R. B. Dahlburg

2016 ◽  
Author(s):  
Daniele Telloni ◽  
Silvia Perri ◽  
Vincenzo Carbone ◽  
Roberto Bruno

2013 ◽  
Vol 764 (1) ◽  
pp. 23 ◽  
Author(s):  
Igor V. Sokolov ◽  
Bart van der Holst ◽  
Rona Oran ◽  
Cooper Downs ◽  
Ilia I. Roussev ◽  
...  

2001 ◽  
Vol 203 ◽  
pp. 456-466
Author(s):  
F. Malara ◽  
M. Velli

Energy release in the solar Corona is characterized by a sequence of space and time localized events, whose intensity follows power-law distributions. In quiet Sun regions, small energy events, possibly under the detection threshold, dominate, thus supporting the “nanoflare” scenario of coronal heating. Two complementar models of heating are discussed, in connection with the above observational features. The first model is based on Alfvénic wavepackets dissipation in 3D force-free magnetic fields; the presence of regions of chaoticity of magnetic lines allows for a fast wave dissipation, within a fraction of a solar radius. The second model describes a MHD turbulence in low-β plasma, in which magnetic energy is continuously furnished by slow photospheric motions. Energy release events corresponds dissipation of current sheets, often associated with magnetic reconnection. The resulting distribution of dissipated power follows a power law, similar to observations.


1999 ◽  
Author(s):  
William H. Matthaeus ◽  
Gary P. Zank ◽  
Sean Oughton

1990 ◽  
Vol 142 ◽  
pp. 215-222
Author(s):  
David Montgomery

Driven, dissipative MHD fluids often seem to undergo relaxation processes. After a turbulent formation phase, a geometrically simpler and less disordered configuration emerges. The best known example is the laboratory reversed-field pinch (RFP); similar field topologies have been proposed for solar prominences and astrophysical “flux ropes.” In a transient situation, the more rapid decay of kinetic and magnetic energy relative to magnetic helicity provides a mechanism for generating an MHD configuration with several similarities to observed RFP states. (This is the Taylor hypothesis, not unrelated to turbulent inverse magnetic cascades.) For the driven steady state, however, all quantities are supplied at the same time-averaged rate at which they are dissipated, by definition; nothing decays relative to anything else. Some other unifying principle, beyond “minimum energy” or “selective decay,” seems necessary to describe the results of driven, steady-state MHD computations. We have been attempting to adapt the principle of minimum energy dissipation rate to MHD. It is a 19th century principle that achieved some success in hydrodynamics and separately in dissipative electrodynamics.


1990 ◽  
Vol 142 ◽  
pp. 207-214
Author(s):  
J. Heyvaerts

Present views on DC current coronal heating are presented. The relation to AC mechanisms, the importance of MHD turbulence in both processes, and the convergence of presently proposed ideas is outlined.


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