Geomagnetic control of equatorial plasma bubble activity modeled by the TIEGCM with <i>Kp</i>

  • B. A. Carter
    Institute for Scientific Research Boston College Newton Massachusetts USA
  • J. M. Retterer
    Institute for Scientific Research Boston College Newton Massachusetts USA
  • E. Yizengaw
    Institute for Scientific Research Boston College Newton Massachusetts USA
  • K. Groves
    Institute for Scientific Research Boston College Newton Massachusetts USA
  • R. Caton
    Air Force Research Laboratory Kirkland AFB Albuquerque New Mexico USA
  • L. McNamara
    Air Force Research Laboratory Kirkland AFB Albuquerque New Mexico USA
  • C. Bridgwood
    Institute for Scientific Research Boston College Newton Massachusetts USA
  • M. Francis
    IPS Radio and Space Services Bureau of Meteorology Sydney New South Wales Australia
  • M. Terkildsen
    IPS Radio and Space Services Bureau of Meteorology Sydney New South Wales Australia
  • R. Norman
    SPACE Research Centre RMIT University Melbourne Victoria Australia
  • K. Zhang
    SPACE Research Centre RMIT University Melbourne Victoria Australia

書誌事項

公開日
2014-08
権利情報
  • http://onlinelibrary.wiley.com/termsAndConditions#vor
DOI
  • 10.1002/2014gl060953
公開者
American Geophysical Union (AGU)

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説明

<jats:title>Abstract</jats:title><jats:p>Describing the day‐to‐day variability of Equatorial Plasma Bubble (EPB) occurrence remains a significant challenge. In this study we use the Thermosphere‐Ionosphere Electrodynamics General Circulation Model (TIEGCM), driven by solar (<jats:italic>F</jats:italic><jats:sub>10.7</jats:sub>) and geomagnetic (<jats:italic>K</jats:italic><jats:italic>p</jats:italic>) activity indices, to study daily variations of the linear Rayleigh‐Taylor (R‐T) instability growth rate in relation to the measured scintillation strength at five longitudinally distributed stations. For locations characterized by generally favorable conditions for EPB growth (i.e., within the scintillation season for that location), we find that the TIEGCM is capable of identifying days when EPB development, determined from the calculated R‐T growth rate, is suppressed as a result of geomagnetic activity. Both observed and modeled upward plasma drifts indicate that the prereversal enhancement scales linearly with <jats:italic>K</jats:italic><jats:italic>p</jats:italic> from several hours prior, from which it is concluded that even small <jats:italic>K</jats:italic><jats:italic>p</jats:italic> changes cause significant variations in daily EPB growth.</jats:p>

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