首页> 外文期刊>Annales Geophysicae >The combined effects of electrojet strength and the geomagnetic activity (IKsubp/sub/I-index) on the post sunset height rise of the F-layer and its role in the generation of ESF during high and low solar activity periods
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The combined effects of electrojet strength and the geomagnetic activity (IKsubp/sub/I-index) on the post sunset height rise of the F-layer and its role in the generation of ESF during high and low solar activity periods

机译:电气强度和地磁活动的组合效应和地磁活动( k p -Index)对F层后的哨所高度升高及其在ESF生成中的作用太阳能活动期高低

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Several investigations have been carried out to identify the factors thatare responsible for the day-to-day variability in the occurrence ofequatorial spread-F (ESF). But the precise forecasting of ESF on aday-to-day basis is still far from reality. The nonlinear development andthe sustenance of ESF/plasma bubbles is decided by the backgroundionospheric conditions, such as the base height of the F-layer (h'F), theelectron density gradient (dN/dz), maximum ionization density (Nmax),geomagnetic activity and the neutral dynamics. There is increasingevidence in the literature during the recent past that shows a welldeveloped Equatorial Ionization Anomaly (EIA) during the afternoon hourscontributes significantly to the initiation of ESF during the post-sunset hours.Also, there exists a good correlation between the Equatorial IonizationAnomaly (EIA) and the Integrated Equatorial ElectroJet (IEEJ) strength, asthe driving force for both is the same, namely, the zonal electric field atthe equator.In this paper, we present a linear relationship that exists between thedaytime integrated equatorial electrojet (IEEJ) strength and the maximumelevated height of the F-layer during post-sunset hours (denoted as peakh'F). An inverse relationship that exists between the 6-h averageKp-index prior to the local sunset and the peak h'F of the F-layer is alsopresented. A systematic study on the combined effects of the IEEJ and theaverage Kp-index on the post-sunset, peak height of the F-layer (peak h'F), whichcontrols the development of ESF/plasma bubbles, is carried out using theionosonde data from an equatorial station, Trivandrum (8.47° N,76.91° E, dip.lat. 0.5° N), an off-equatorial station, SHAR(13.6° N, 79.8° E, dip.lat. 10.8° N) and VHF scintillations (244 MHz)observed over a nearby low-latitude station, Waltair (17.7° N,83.3° E, dip.lat. 20° N). From this study, it has been found thatthe threshold base height of the F-layer at the equator for the developmentof plasma bubbles is reduced from 405 km to 317 km as the solar activitydecreases from March 2001 (mean Rz=113.5) to March 2005 (mean Rz=24.5).This decrease in threshold height with the decreasing solar activity isexplained on the basis of changes in the local linear growth rate ofthe collisional Rayleigh-Taylor instability, due to the variability of variousterms such as inverse density gradient scale length (L−1), ion-neutralcollision frequency (νin) and recombination rate (R) with thechanges in the solar activity.
机译:已经进行了几项调查,以确定对常见差异(ESF)发生的日常变异性的因素。但对ASF的确切预测仍然远离现实。非线性发育和ESF /等离子气泡的寄托由背景推动的条件决定,例如F层的基础高度( H'f ),电子密度梯度(DN / DZ),最大电离密度( n max ),地磁活动和中性动力学。在最近的过去,文献中的文献越来越多地显示出在午后的赤道电离异常(EIA)在日落后时期的启动中,在日落后的时间内显着扩张。赤道离子化(EIA)之间存在良好的相关性(EIA )和综合赤道电气喷射(IEEJ)强度,两者的驱动力是相同的,即赤道的区域电场。 在本文中,我们呈现了在eDaytime综合赤道之间存在的线性关系在日落后时期的电气喷射(IEEJ)强度和F层的最终高度(表示为峰值 h'f )。在局部日落之前的6-h平均值 k p -index之间存在的反比关系,并且f的峰值 h'f - 层是alsupresented。对IEEJ和胸腺素的组合效应的系统研究 k p -index在日落后,F层的峰值高度(峰值 h' f ),使用来自赤道站的IhiOnonde数据,Trivandrum(8.47°N,76.91°E,Dip.lat。0.5°N),进行ISF /等离子气泡的开发,进行ESF /等离子气泡的开发。在附近的低纬度站,沃尔航站(17.7°N,83.3°E,Dip.lat)观察到,SHAR(13.6°N,DIP.LAT。10.8°N)和VHF闪烁(244 MHz)观察到。 20°N)。从该研究开始,已经发现,随着来自2001年3月的太阳能活性分泌,等离子体泡沫的赤道在赤道中的F层的阈值底部高度从405 km减少到317 km(平均值 rz = 113.5)至2005年3月(平均值 rz = 24.5)。这对阈值高度降低了阈值高度,在局部线性增长速度的局部线性生长速度的变化基础上,由于攻击的瑞利 - 泰勒不稳定性的变化而降低诸如逆密度梯度刻度长度(L -1 / sup>),离子 - 中性可团频率(在中的ν )和复合速率的变异性(r)在太阳能活动中有TheChanges。

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