Three dimensional MHD simulations for an emerging twisted magnetic flux tube

Author(s):  
T.M. Miyagoshi ◽  
T.Y. Yokoyama
1996 ◽  
Vol 466 (1) ◽  
pp. L39-L42 ◽  
Author(s):  
T. Amari ◽  
J. F. Luciani ◽  
J. J. Aly ◽  
M. Tagger

2001 ◽  
Vol 548 (1) ◽  
pp. L69-L72 ◽  
Author(s):  
Geoffrey V. Bicknell ◽  
Jianke Li

2012 ◽  
Vol 64 (5) ◽  
pp. L4 ◽  
Author(s):  
Tetsuya Magara ◽  
Jun-Mo An ◽  
Hwanhee Lee ◽  
Jihye Kang ◽  
Satoshi Inoue ◽  
...  

2001 ◽  
Vol 203 ◽  
pp. 225-228
Author(s):  
W. P. Abbett ◽  
G. H. Fisher ◽  
Y. Fan

Over the past decade, “thin flux tube” models have proven successful in explaining many properties of active regions in terms of magnetic flux tube dynamics in the solar interior. On the other hand, recent 2-D MHD simulations of the emergence of magnetic flux have shown that many of the assumptions adopted in the thin flux tube approximation are invalid. For example, unless the flux tubes exhibit a large degree of initial field line twist — and observations of emerging active regions suggest they do not — they will fragment (break apart) before they are able to emerge through the surface. We attempt to resolve this paradox using a number of 3-D MHD simulations (in the anelastic approximation) that describe the rise and fragmentation of twisted magnetic flux tubes. We find that the degree of fragmentation of an evolving Ω-loop depends strongly on the 3-D geometry of the loop, and that the Coriolis force plays a dynamically important role in the evolution and emergence of magnetic flux.


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