SIMULATIONS OF EMERGING MAGNETIC FLUX. II. THE FORMATION OF UNSTABLE CORONAL FLUX ROPES AND THE INITIATION OF CORONAL MASS EJECTIONS

被引:65
作者
Leake, James E. [1 ]
Linton, Mark G. [2 ]
Antiochos, Spiro K. [3 ]
机构
[1] George Mason Univ, Coll Sci, Fairfax, VA 22030 USA
[2] US Naval Res Lab, Washington, DC 20375 USA
[3] NASA, Goddard Space Flight Ctr, Greenbelt, MD 20711 USA
关键词
magnetohydrodynamics (MHD); Sun: atmosphere; Sun: coronal mass ejections (CMEs); Sun: flares; Sun: magnetic fields; EMERGENCE; MODEL; ERUPTION; RECONNECTION; MORPHOLOGY; EVOLUTION; TOPOLOGY; PLASMA; DRIVEN; TUBE;
D O I
10.1088/0004-637X/787/1/46
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present results from three-dimensional magnetohydrodynamic simulations of the emergence of a twisted convection zone flux tube into a pre-existing coronal dipole field. As in previous simulations, following the partial emergence of the sub-surface flux into the corona, a combination of vortical motions and internal magnetic reconnection forms a coronal flux rope. Then, in the simulations presented here, external reconnection between the emerging field and the pre-existing dipole coronal field allows further expansion of the coronal flux rope into the corona. After sufficient expansion, internal reconnection occurs beneath the coronal flux rope axis, and the flux rope erupts up to the top boundary of the simulation domain (similar to 36 Mm above the surface). We find that the presence of a pre-existing field, orientated in a direction to facilitate reconnection with the emerging field, is vital to the fast rise of the coronal flux rope. The simulations shown in this paper are able to self-consistently create many of the surface and coronal signatures used by coronal mass ejection (CME) models. These signatures include surface shearing and rotational motions, quadrupolar geometry above the surface, central sheared arcades reconnecting with oppositely orientated overlying dipole fields, the formation of coronal flux ropes underlying potential coronal field, and internal reconnection which resembles the classical flare reconnection scenario. This suggests that proposed mechanisms for the initiation of a CME, such as "magnetic breakout", are operating during the emergence of new active regions.
引用
收藏
页数:13
相关论文
共 38 条
  • [1] A twisted flux rope model for coronal mass ejections and two-ribbon flares
    Amari, T
    Luciani, JF
    Mikic, Z
    Linker, J
    [J]. ASTROPHYSICAL JOURNAL, 2000, 529 (01) : L49 - L52
  • [2] Coronal mass ejection: Initiation, magnetic helicity, and flux ropes. I. Boundary motion driven evolution
    Amari, T
    Luciani, JF
    Aly, JJ
    Mikic, Z
    Linker, J
    [J]. ASTROPHYSICAL JOURNAL, 2003, 585 (02) : 1073 - 1086
  • [3] The magnetic topology of solar eruptions
    Antiochos, SK
    [J]. ASTROPHYSICAL JOURNAL, 1998, 502 (02) : L181 - L184
  • [4] A model for solar coronal mass ejections
    Antiochos, SK
    DeVore, CR
    Klimchuk, JA
    [J]. ASTROPHYSICAL JOURNAL, 1999, 510 (01) : 485 - 493
  • [5] Emergence of magnetic flux from the convection zone into the corona
    Archontis, V
    Moreno-Insertis, F
    Galsgaard, K
    Hood, AW
    O'Shea, E
    [J]. ASTRONOMY & ASTROPHYSICS, 2004, 426 (03): : 1047 - 1063
  • [6] Magnetic flux emergence: a precursor of solar plasma expulsion
    Archontis, V.
    Hood, A. W.
    [J]. ASTRONOMY & ASTROPHYSICS, 2012, 537
  • [7] Flux emergence and coronal eruption
    Archontis, V.
    Hood, A. W.
    [J]. ASTRONOMY & ASTROPHYSICS, 2010, 514
  • [8] Eruption of magnetic flux ropes during flux emergence
    Archontis, V.
    Torok, T.
    [J]. ASTRONOMY & ASTROPHYSICS, 2008, 492 (02): : L35 - L38
  • [9] Sigmoidal morphology and eruptive solar activity
    Canfield, RC
    Hudson, HS
    Mckenzie, DE
    [J]. GEOPHYSICAL RESEARCH LETTERS, 1999, 26 (06) : 627 - 630
  • [10] Carmichael H., 1964, NASA Special Publication, V50, P451