4.6 Article

Emergence of non-twisted magnetic fields in the Sun: Jets and atmospheric response

期刊

ASTRONOMY & ASTROPHYSICS
卷 584, 期 -, 页码 -

出版社

EDP SCIENCES S A
DOI: 10.1051/0004-6361/201423781

关键词

Sun: activity; Sun: interior; Sun: magnetic fields; magnetohydrodynamics (MHD); methods: numerical

资金

  1. EU [IEF-272549]
  2. Royal Society
  3. European Union (European Social Fund-ESF)
  4. Greek national funds through the Operational Program Education and Lifelong Learning of the National Strategic Reference Framework (NSRF) - Research Funding Program: Thales
  5. Program IKY Scholarships of the Greek national funds through the Operational Program Education and Lifelong Learning of the NSRF through the European Social Fund of ESPA
  6. SOLARNET project - European Commisions FP7 Capacities Program [312495]
  7. STFC
  8. SRIF
  9. Science and Technology Facilities Council [ST/H001964/1] Funding Source: researchfish
  10. STFC [ST/H001964/1] Funding Source: UKRI

向作者/读者索取更多资源

Aims. We study the emergence of a non-twisted flux tube from the solar interior into the solar atmosphere. We investigate whether the length of the buoyant part of the flux tube (i.e. lambda) affects the emergence of the field and the dynamics of the evolving magnetic flux system. Methods. We perform three-dimensional (3D), time-dependent, resistive, compressible magnetohydrodynamic (MHD) simulations using the Lare3D code. Results. We find that there are considerable differences in the dynamics of the emergence of a magnetic flux tube when lambda is varied. In the solar interior, for larger values of lambda, the rising magnetic field emerges faster and expands more due to its lower magnetic tension. As a result, its field strength decreases and its emergence above the photosphere occurs later than in the smaller lambda case. However, in both cases, the emerging field at the photosphere becomes unstable in two places, forming two magnetic bipoles that interact dynamically during the evolution of the system. Most of the dynamic phenomena occur at the current layer, which is formed at the interface between the interacting bipoles. We find the formation and ejection of plasmoids, the onset of successive jets from the interface, and the impulsive heating of the plasma in the solar atmosphere. We discuss the triggering mechanism of the jets and the atmospheric response to the emergence of magnetic flux in the two cases.

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