Sequential Eruptions Triggered by Flux Emergence: Observations and Modeling

被引:16
作者
Dacie, S. [1 ]
Torok, T. [2 ]
Demoulin, P. [3 ]
Linton, M. G. [4 ]
Downs, C. [2 ]
van Driel-Gesztelyi, L. [1 ,3 ,5 ]
Long, D. M. [1 ]
Leake, J. E. [6 ]
机构
[1] Univ Coll London, Mullard Space Sci Lab, Holmbury RH5 6NT, Surrey, England
[2] Predict Sci Inc, 9990 Mesa Rim Rd,Suite 170, San Diego, CA 92121 USA
[3] CNRS, UMR 8109, Observat Paris, LESIA, F-92195 Meudon, France
[4] Naval Res Lab, Washington, DC 20375 USA
[5] Hungarian Acad Sci, Konkoly Observ, Budapest, Hungary
[6] NASA, Goddard Space Flight Ctr, 8800 Greenbelt Rd, Greenbelt, MD 20771 USA
关键词
Sun: corona; Sun: coronal mass ejections (CMEs); Sun: magnetic fields; CORONAL MASS EJECTIONS; MAGNETIC-FLUX; EMERGING FLUX; FILAMENT ERUPTIONS; BREAKOUT MODEL; SOLAR-FLARES; RECONNECTION; INITIATION; SIMULATIONS; TONGUES;
D O I
10.3847/1538-4357/aacce3
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We describe and analyze observations by the Solar Dynamics Observatory of the emergence of a small, bipolar active region within an area of unipolar magnetic flux that was surrounded by a circular, quiescent filament. Within only 8 hours from the start of the emergence, a partial splitting of the filament and two consecutive coronal mass ejections took place. We argue that all three dynamic events occurred as a result of particular magnetic-reconnection episodes between the emerging bipole and the pre-existing coronal magnetic field. To substantiate our interpretation, we consider 3D magnetohydrodynamic simulations that model the emergence of magnetic flux in the vicinity of a large-scale coronal flux rope. The simulations qualitatively reproduce most of the reconnection episodes suggested by the observations, as well as the filament splitting, the first eruption, and the formation of sheared/twisted fields that may have played a role in the second eruption. Our results suggest that the position of emerging flux with respect to the background magnetic configuration is a crucial factor for the resulting evolution, while previous results suggest that parameters such as the orientation or the amount of emerging flux are important as well. This poses a challenge for predicting the onset of eruptions that are triggered by flux emergence, and calls for a detailed survey of the relevant parameter space by means of numerical simulations.
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页数:11
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共 50 条
[1]   A staggered grid, Lagrangian-Eulerian remap code for 3-D MHD simulations [J].
Arber, TD ;
Longbottom, AW ;
Gerrard, CL ;
Milne, AM .
JOURNAL OF COMPUTATIONAL PHYSICS, 2001, 171 (01) :151-181
[2]  
Aulanier G., 2014, IAU S, V300, P184
[3]   The large angle spectroscopic coronagraph (LASCO) [J].
Brueckner, GE ;
Howard, RA ;
Koomen, MJ ;
Korendyke, CM ;
Michels, DJ ;
Moses, JD ;
Socker, DG ;
Dere, KP ;
Lamy, PL ;
Llebaria, A ;
Bout, MV ;
Schwenn, R ;
Simnett, GM ;
Bedford, DK ;
Eyles, CJ .
SOLAR PHYSICS, 1995, 162 (1-2) :357-402
[4]  
Carmichael H., 1964, NASA Special Publication, V50, P451
[5]   An emerging flux trigger mechanism for coronal mass ejections [J].
Chen, PF ;
Shibata, K .
ASTROPHYSICAL JOURNAL, 2000, 545 (01) :524-531
[6]   Magnetic free energies of breakout coronal mass ejections [J].
DeVore, CR ;
Antiochos, SK .
ASTROPHYSICAL JOURNAL, 2005, 628 (02) :1031-1045
[7]   Coronal flux rope catastrophe caused by photospheric flux emergence [J].
Ding, J. Y. ;
Hu, Y. Q. .
ASTROPHYSICAL JOURNAL, 2008, 674 (01) :554-559
[8]   The initiation of coronal mass ejections by magnetic flux emergence [J].
Dubey, G. ;
van der Holst, B. ;
Poedts, S. .
ASTRONOMY & ASTROPHYSICS, 2006, 459 (03) :927-934
[9]   THE INITIATION OF CORONAL MASS EJECTIONS BY NEWLY EMERGING MAGNETIC-FLUX [J].
FEYNMAN, J ;
MARTIN, SF .
JOURNAL OF GEOPHYSICAL RESEARCH-SPACE PHYSICS, 1995, 100 (A3) :3355-3367
[10]   Eruption of a multiple-turn helical magnetic flux tube in a large flare: Evidence for external and internal reconnection that fits the breakout model of solar magnetic eruptions [J].
Gary, GA ;
Moore, RL .
ASTROPHYSICAL JOURNAL, 2004, 611 (01) :545-556