Helioseismically determined near-surface flows underlying a quiescent filament

被引:25
|
作者
Hindman, Bradley W. [1 ]
Haber, Deborah A.
Toomre, Juri
机构
[1] Univ Colorado, Joint Inst Lab Astrophys, Boulder, CO 80309 USA
[2] Univ Colorado, Dept Astrophys & Planetary Sci, Boulder, CO 80309 USA
来源
ASTROPHYSICAL JOURNAL | 2006年 / 653卷 / 01期
关键词
Sun : filaments; Sun : helioseismology;
D O I
10.1086/508603
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The extended filaments seen in Ha images of the solar disk, and the corresponding prominences when viewed at the solar limb, are one of the great hallmarks of solar magnetism. Such arches of magnetic field and the coronal plasma structures they support are both beautiful and enigmatic. Many models of filament fort-nation and maintenance invoke the existence of surface plasma flows, which are used to drive the magnetic reconnection needed to form twisted loops of flux held down by a coronal arcade. These flows are typically composed of a converging flow, which brings flux elements of opposite polarity together, combined with a tangential shear that stresses the coronal arcade. In this paper we present helioseismic measurements of near-surface flows underlying a single quiescent filament lying within a decayed active region. Newly devised high-resolution ring analyses (HRRA) with both 2 degrees and 4 degrees spatial resolution were applied to Doppler imaging data provided by the Michelson Doppler Imager (MDI) instrument on the SOHO spacecraft. A long-lived filament appearing in 2002 May and April was studied. We find that the filament channel is a region of vigorous subphotospheric convection. The largest observed scales of such convection span the region of weak magnetic field separating the active region's two polarities. Thus, the magnetic neutral line that forms the spine of the filament channel tends to lie along the centers of large convection cells. In temporal and spatial averages of the flow field, we do not find a systematic converging flow. However, we do detect a significant shearing flow parallel to the neutral line. This shear takes the form of two oppositely directed jets, on I e to either side of the neutral line and within 20 Mm of the line. The jets produce a net shear in the flow speed of 30 m s(-1) occurring over a distance of 20 Mm.
引用
收藏
页码:725 / 732
页数:8
相关论文
共 50 条
  • [21] Imaging the Sun's Near-surface Flows Using Mode-coupling Analysis
    Mani, Prasad
    Hanson, Chris S.
    Hanasoge, Shravan
    ASTROPHYSICAL JOURNAL, 2022, 926 (02):
  • [22] Time-distance helioseismology with f modes as a method for measurement of near-surface flows
    Duvall, TL
    Gizon, L
    SOLAR PHYSICS, 2000, 192 (1-2) : 177 - 191
  • [23] Near-surface electromagnetic surveying
    Dawoud, Mohamed
    Hallinan, Stephen
    Herrmann, Rolf
    Van Kleef, Frank
    Oilfield Review, 2009, 21 (01): : 20 - 25
  • [24] NEAR-SURFACE DEFECT DETECTION
    MUCCIARDI, AN
    SHANKAR, R
    MATERIALS EVALUATION, 1981, 39 (01) : 74 - 77
  • [25] Shallow near-surface effects
    Krohn, Christine E.
    Murray, Thomas J.
    GEOPHYSICS, 2016, 81 (05) : T221 - T231
  • [26] Advances in near-surface seismology
    Baker, Gregory S.
    Gilcrist, Laura E.
    Gaines, David P.
    NEAR-SURFACE GEOPHYSICS AND HUMAN ACTIVITY, 2008, : 62 - 66
  • [27] Near-surface anisotropic turbulence
    Klipp, Cheryl
    ATMOSPHERIC PROPAGATION VII, 2010, 7685
  • [28] MICROTREMORS, A NEAR-SURFACE PHENOMENON?
    Nieto, D.
    Baradello, L.
    Kaka, S. I.
    Vesnaver, A.
    JOURNAL OF SEISMIC EXPLORATION, 2011, 20 (04): : 379 - 398
  • [29] The near-surface evening transition
    Mahrt, L.
    QUARTERLY JOURNAL OF THE ROYAL METEOROLOGICAL SOCIETY, 2017, 143 (708) : 2940 - 2948
  • [30] LUNAR NEAR-SURFACE STRUCTURE
    COOPER, MR
    KOVACH, RL
    WATKINS, JS
    REVIEWS OF GEOPHYSICS, 1974, 12 (03) : 291 - 308