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首页> 外文期刊>Annales Geophysicae >Comparison of the measured and modeled electron densities, and electron and ion temperatures in the low-latitude ionosphere during 19-21 March 1988
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Comparison of the measured and modeled electron densities, and electron and ion temperatures in the low-latitude ionosphere during 19-21 March 1988

机译:1988年3月19日至21日在低纬度电离层中测量和模拟的电子密度以及电子和离子温度的比较

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We have presented a comparison between the modeled NmF2 andhmF2, and NmF2 and hmF2 which were observed at the equatorial anomaly crestand close to the geomagnetic equator simultaneously by the Akita, Kokubunji,Yamagawa, Okinawa, Chung-Li, Manila, Vanimo, and Darwin ionospheric soundersand by the middle and upper atmosphere (MU) radar at Shigaraki(34.85°N, 136.10°E, Japan) during the 19-21 March 1988geomagnetically quiet time period at moderate solar activity nearapproximately the same geomagnetic meridian of 201°. A comparisonbetween the electron, Te, and ion, Ti, temperatures measured bythe MU radar and those produced by the model of the ionosphere andplasmasphere is presented for 19-21 March 1988. It is shown that there isa large disagreement between the measured and modeled hmF2 from about07:00 UT to about 11:00 UT if the equatorial ExB drift given byScherliess and Fejer (1999) is used. The required equatorial upward ExB drift is weaker from 03:14 UT to 11:14 UT than that given by Scherliessand Fejer (1999) for the studied time period. The required modification ofthe ExB drift weakens the effect of the fountain in NmF2 bringing themodeled and measured hmF2 and NmF2, into reasonable agreement. The depth ofthe equatorial NmF2 trough in the calculated NmF2 is approximatelyconsistent with the measured depth if the modified equatorial ExB drift is used. It has been found that the north-south asymmetries in theobserved NmF2 and hmF2 about the geomagnetic equator are mainly caused bythe asymmetry in the neutral wind about the geomagnetic equator. In theNorthern Hemisphere, the meridional neutral wind taken from the HWW90 windmodel and the NRLMSISE-00 atomic oxygen density are corrected so that themodel results agree with the ionospheric sounders and MU radar observations.A theory of the primary mechanisms causing the latitude dependence of themorning and evening peaks in Te is developed. The latitude dependenceof the magnitudes of these peaks in Te is interpreted in terms ofthe corresponding dependence of the electron density. The relative role ofthe ExB drift and the plasma drift caused by the neutral wind in theformation and the dependence of the magnitudes of the morning andevening electron temperature peaks on the geomagnetic latitude is studied.
机译:我们已经提出了模型化的NmF2和hmF2以及NmF2和hmF2的比较,秋田,国分文治,山川,冲绳,中kin,马尼拉,瓦尼莫和达尔文电离层同时在赤道异常赤道处靠近地磁赤道观测到1988年3月19日至21日在滋贺木县(34.85°N,136.10°E,日本)的中高层大气(MU)雷达探测到的地磁静默时间段,在中等太阳活动下,地磁子午线接近于201°。给出了3月19日至21日由MU雷达测量的电子T e 和离子T i 与由电离层和等离子层模型产生的温度之间的比较。 1988年。研究表明,如果赤道 E x <,从大约07:00 UT到大约11:00 UT,测得的和模拟的hmF2之间存在很大的分歧。使用Scherliess和Fejer(1999)给出的i> B 漂移。从03:14 UT到11:14 UT所需的赤道向上 E x B 漂移比Scherliessand Fejer(1999)给出的研究时间段。对 E x B 漂移的必要修改会削弱NmF2中源泉的影响,从而使建模和测量的hmF2和NmF2,达成合理协议。如果修改后的赤道 E x B ,则计算出的NmF2中赤道NmF2谷的深度与测得的深度大致一致。 >使用漂移。已经发现,在地磁赤道附近观测到的NmF2和hmF2的南北不对称性主要是由在地磁赤道周围的中性风的不对称性引起的。在北半球,对从HWW90风模型和NRLMSISE-00原子氧密度获取的子午中风进行了校正,使模型结果与电离层测深仪和MU雷达观测结果相吻合。 T e 出现了傍晚高峰。 T e 中这些峰的大小的纬度依赖性是根据电子密度的相应依赖性来解释的。 E x B 漂移与中性风引起的等离子体漂移的相对作用及其相关性研究了地磁纬度上早晚电子温度峰值的大小。

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