首页> 外文期刊>Journal of atmospheric and solar-terrestrial physics >The ionospheric F2-region at low geomagnetic latitudes during the geomagnetic storms of 22–26 April 1990: Comparison of observed and modeled response
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The ionospheric F2-region at low geomagnetic latitudes during the geomagnetic storms of 22–26 April 1990: Comparison of observed and modeled response

机译:在1990年4月22日至26日的地磁风暴中低地磁纬度的电离层F2区域:观测到的响应和模拟响应的比较

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A comparison between the modeled NmF2 and hmF2 and NmF2 and hmF2, which were observed by the Kokubunji, Okinawa, Manila, Vanimo, and Darwin ionospheric sounders and by the middle and upper (MU) atmosphere radar, have been used to study the time-dependent response of the low-latitude ionosphere to geomagnetic forcing during a time series of geomagnetic storms from 22 to 26 April 1990. The reasonable agreement between the model results and data requires the modified equatorial meridional E×B plasma drift, the modified HWM90 wind, and the modified NRLMSISE-00 neutral densities. We found that changes in a flux of plasma into the nighttime equatorial F2-region from higher L-shells to lower L-shells caused by the meridional component of the E×B plasma drift lead to enhancements in NmF2 close to the geomagnetic equator. The equatorward wind-induced plasma drift along magnetic field lines, which cross the Earth equatorward of about 20° geomagnetic latitude in the northern hemisphere and about ?19° geomagnetic latitude in the southern hemisphere, contributes to the maintenance of the F2-layer close to the geomagnetic equator. The nighttime weakening of the equatorial zonal electric field (in comparison with that produced by the empirical model of Fejer and Scherliess [Fejer, B.G., Scherliess, L., 1997. Empirical models of storm time equatorial zonal electric fields. J. Geophys. Res. 102, 24047–24056] or Scherliess and Fejer [Scherliess, L., Fejer, B.G., 1999. Radar and satellite global equatorial F region vertical drift model. J. Geophys. Res. 104, 6829–6842) in combination with corrected equatorward nighttime wind-induced plasma drift along magnetic field lines in the both geomagnetic hemispheres are found to be the physical mechanism of the nighttime NmF2 enhancement formation close to the geomagnetic equator over Manila during 22–26 April 1990. The model crest-to-trough ratios of the equatorial anomaly are used to study the relative role of the main mechanisms of the equatorial anomaly suppression for the 22–26 April 1990 geomagnetic storms. During the most part of the studied time period, a total contribution from geomagnetic storm disturbances in the neutral temperature and densities to the equatorial anomaly changes is less than that from meridional neutral winds and variations in the E×B plasma drift. It is shown that the latitudinal positions of the crests are determined by the E×B drift velocity and the neutral wind velocity.
机译:Kokubunji,冲绳,马尼拉,Vanimo和达尔文电离层测深仪以及中高层(MU)大气雷达观测到的模拟NmF2和hmF2以及NmF2和hmF2之间的比较已用于研究时间-在1990年4月22日至26日的一系列地磁风暴中,低纬度电离层对地磁强迫的响应。模型结果与数据之间的合理吻合需要改进的赤道子午线E×B等离子体漂移,改进的HWM90风,以及修改后的NRLMSISE-00中性密度。我们发现,由E×B等离子体漂移的子午分量引起的,从较高的L壳到较低的L壳进入夜间赤道F2区域的等离子体通量的变化导致靠近地磁赤道的NmF2增强。赤道风诱发的等离子体沿磁场线漂移,在北半球约20°地磁纬度和南半球约19°地磁纬度横越地球赤道,有助于维持F2层接近地磁赤道。夜间赤道纬向电场减弱(与Fejer和Scherliess的经验模型[Fejer,BG,Scherliess,L.,1997.风暴时间赤道纬向电场的经验模型比较。J。Geophys。Res 。102,24047–24056]或Scherliess and Fejer [Scherliess,L.,Fejer,BG,1999.雷达和卫星全球赤道F区垂直漂移模型。J. Geophys。Res。104,6829–6842),并结合校正在1990年4月22日至26日,马尼拉上空靠近地磁赤道的夜间NmF2增强形成的物理机制被认为是沿两个地磁半球沿磁力线的赤道夜间风诱发的等离子体漂移的物理机制。利用赤道异常比率来研究1990年4月22日至26日地磁风暴对赤道异常抑制的主要机制的相对作用。在研究的大部分时间里,中性温度和密度的地磁风暴扰动对赤道异常变化的总贡献小于经线中性风和E×B等离子体漂移变化的总贡献。结果表明,波峰的纬度位置由E×B漂移速度和中性风速确定。

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