scholarly journals From Solar and Stellar Flares to Coronal Heating: Theory and Observations of How Magnetic Reconnection Regulates Coronal Conditions

2008 ◽  
Vol 676 (1) ◽  
pp. L69-L72 ◽  
Author(s):  
P. A. Cassak ◽  
D. J. Mullan ◽  
M. A. Shay
1999 ◽  
Vol 524 (1) ◽  
pp. L75-L78 ◽  
Author(s):  
P. A. Sturrock ◽  
C. B. Roald ◽  
R. Wolfson

2005 ◽  
Vol 12 (1) ◽  
pp. 012904 ◽  
Author(s):  
Rekha Jain ◽  
Philippa Browning ◽  
K. Kusano

2000 ◽  
Vol 538 (2) ◽  
pp. 960-967 ◽  
Author(s):  
Colin B. Roald ◽  
P. A. Sturrock ◽  
Richard Wolfson

2004 ◽  
Vol 219 ◽  
pp. 159-170 ◽  
Author(s):  
Manuel Güdel

Coronal structure and coronal heating are intimately related in magnetically active stars. Coronal structure is commonly inferred from radio interferometry and from eclipse and rotational modulation studies. We discuss to what extent flares may be responsible for coronal structure and global observable properties in magnetically active stars.


2008 ◽  
Vol 4 (S259) ◽  
pp. 191-200
Author(s):  
Lidia van Driel-Gesztelyi

AbstractMagnetic reconnection is thought to play an important role in liberating free energy stored in stressed magnetic fields. The consequences vary from undetectable nanoflares to huge flares, which have signatures over a wide wavelength range, depending on e.g. magnetic topology, free energy content, total flux, and magnetic flux density of the structures involved. Events of small energy release, which are thought to be the most numerous, are one of the key factors in the existence of a hot corona in the Sun and solar-like stars. The majority of large flares are ejective, i.e. involve the expulsion of large quantities of mass and magnetic field from the star. Since magnetic reconnection requires small length-scales, which are well below the spatial resolution limits of even the solar observations, we cannot directly observe magnetic reconnection happening. However, there is a plethora of indirect evidences from X-rays to radio observations of magnetic reconnection. I discuss key observational signatures of flares on the Sun and solar-paradigm stellar flares and describe models emphasizing synergy between observations and theory.


1996 ◽  
Vol 237 (1-2) ◽  
pp. 49-73 ◽  
Author(s):  
Eric R. Priest

2009 ◽  
Vol 506 (2) ◽  
pp. 913-925 ◽  
Author(s):  
A. W. Hood ◽  
P. K. Browning ◽  
R. A. M. Van der Linden

2010 ◽  
Vol 6 (S274) ◽  
pp. 10-17
Author(s):  
Masaaki Yamada ◽  
Hantao Ji

Magnetic reconnection (Parker, 1957; Sweet, 1958; Petschek, 1964; Yamada et al., 2010; Biskamp, 2000; Tsuneta, 1996; Kivelson and Russell, 1995; Yamada, 2007; Birn et al., 2001; Drake et al., 2003) is considered important to many astrophysical phenomena including stellar flares, magnetospheric disruptions of magnetars, and dynamics of galactic lobes. Research on magnetic reconnection started with observations in solar coronae and in the Earths magnetosphere, and a classical theory was developed based on MHD. Recent progress has been made by understanding the two-fluid physics of reconnection, through space and astrophysical observations (Tsuneta, 1996; Kivelson and Russell, 1995), laboratory experiments (Yamada, 2007), and theory and numerical simulations (Birn et al., 2001; Daughton et al., 2006; Uzdensky and Kulsrud, 2006). Laboratory experiments dedicated to the study of the fundamental reconnection physics have tested the physics mechanisms and their required conditions, and have provided a much needed bridge between observations and theory. For example, the Magnetic Reconnection Experiment (MRX) experiment (http://mrx.pppl.gov) has rigorously cross-checked the leading theories though quantitative comparisons of the numerical simulations and space astrophysical observations (Mozer et al., 2002). Extensive data have been accumulated in a wide plasma parameter regime with Lundquist numbers of S = 100 − 3000, where S is a ratio of the magnetic diffusion time to the Alfven transit time.


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