A PHYSICAL MODEL FOR IONOSPHERIC VERTICAL PROFILE AND COMPARISON BETWEEN IT AND IRI-90
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摘要: 在80-500km范围内考虑了3种中性成份的4种离子,从严格的电子和离子密度连续方程出发,对中性风和扩散效应进行了全面、连续的考虑,由此建立了一种电离层的物理模式;在此模式的基础上针对北京地区分别对太阳活动低年(F10.7=60)、高年(F10.7=300)的春(DOY=90)、夏(DOY=180)、秋(DOY=270)、冬(DOY=365)进行计算,并将所得结果与IRI-90进行了比较.结果表明: E层为典型的Chapman层: E-F谷区深度一般为0.2-0.5之间,比IRI要深;F1缘在太阳活动低年的四季都出现,其中夏天最明显,已形成了一个F1层,冬天最不明显,仅表现为一个轻微的凸缘,在太阳活动高年只有夏天出现了F1凸缘,这与现有理论相符合,而IRI-90较少出现明显的F1缘;F2层的电子密度是活动高年比低年大,平均冬天比夏天大,这与观测结果也基本符合.Abstract: A physical model for ionospheric vertical profile is established, taking into ac-count four species of ions and electrons in the region of 80-500 km. Neutral windand ions' motion are both involved in the continuity equations for those five species.Ionospheric proflles in different seasons at low and high solar activities are calcu-lated and compared with the results from IRI-90. Results show that E region is atypical Chapman layer and the depth of E-F valley is generally 0.2-0.5 which isdeeper than that given by IRI-90. That the F1 ledge is most obvious in summerat low solar activity is consistent with widely accepted theories, but the F1 ledgeseldom appear in IRI-90. In F2 region, the electron number density at high solaractivity is greater than that at low solar activity, and in winter is greater than thatin summer. rhese all agree with observations rather well.
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Key words:
- Ionospheric model /
- E-F valley /
- F1 ledge /
- IRI-90
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