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首页> 外文期刊>Annales Geophysicae >The combined effects of electrojet strength and the geomagnetic activity (K_p-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 (K_p-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:电喷强度和地磁活动(K_p-index)对F层日落后高度升高的综合影响及其在太阳活动高低期期间在ESF产生中的作用

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摘要

Several investigations have been carried out to identify the factors that are responsible for the day-to-day variability in the occurrence of equatorial spread-F (ESF). But the precise forecasting of ESF on a day-to-day basis is still far from reality. The nonlinear development and the sustenance of ESF/plasma bubbles is decided by the background ionospheric conditions, such as the base height of the F-layer (h′F), the electron density gradient (dN/dz), maximum ion ization density (Nmax), geomagnetic activity and the neutral dynamics. There is increasing evidence in the literature during the recent past that shows a well developed Equatorial Ionization Anomaly (EIA) during the afternoon hours contributes significantly to the initiation of ESF during the post sunset hours. Also, there exists a good correlation between the Equatorial Ionization Anomaly (EIA) and the Integrated Equatorial ElectroJet (IEEJ) strength, as the driving force for both is the same, namely, the zonal electric field at the equator. In this paper, we present a linear relationship that exists between the daytime integrated equatorial electrojet (IEEJ) strength and the maximum elevated height of the F-layer during post-sunset hours (denoted as peak h′F). An inverse relationship that exists between the 6-h average K_p-index prior to the local sunset and the peak h′F of the F-layer is also presented. A systematic study on the combined effects of the IEEJ and the average K_p-index on the post-sunset, peak height of the F-layer (peak h′F), which controls the development of ESF/plasma bubbles, is carried out using the ionosonde 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 scintilla- tions (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 that the threshold base height of the F-layer at the equator for the development of plasma bubbles is reduced from 405 km to 317 km as the solar activity decreases from March 2001 (mean Rz=113.5) to March 2005 (mean Rz=24.5). This decrease in threshold height with the decreasing solar activity is explained on the basis of changes in the local linear growth rate of the collisional Rayleigh-Taylor instability, due to the variability of various terms such as inverse density gradient scale length (L~(-1)), ion-neutral collision frequency (v_in) and recombination rate (R) with the changes in the solar activity.
机译:已经进行了几项调查,以确定造成赤道传播F(ESF)的日常变化的因素。但是,每天对ESF进行精确的预测仍然远远不能实现。 ESF /等离子气泡的非线性发展和维持取决于背景电离层条件,例如F层的基础高度(h'F),电子密度梯度(dN / dz),最大离子化密度( Nmax),地磁活动和中性动力学。在最近的文献中,越来越多的证据表明,下午时段赤道电离异常(EIA)的发展十分完善,这在日落后时段对ESF的启动起了重要作用。而且,由于两者的驱动力相同,即赤道处的纬向电场,因此在赤道电离异常(EIA)和综合赤道电喷(IEEJ)强度之间存在良好的相关性。在本文中,我们提出了日间集成赤道电喷(IEEJ)强度与日落后小时F层的最大升高高度之间的线性关系(称为峰h'F)。还提出了在局部日落之前的6小时平均K_p指数与F层的峰值h'F之间存在反比关系。系统地研究了IEEJ和平均K_p指数对控制ESF /血浆气泡发展的日落后F层的峰高(峰值h'F)的影响。来自赤道站特里凡得琅(8.47°N,76.91°E,倾角0.5°N),赤道站SHAR(13.6°N,79.8°E,倾角10.8°N)的离子探空仪数据)和在附近的低纬度站Waltair(北纬17.7°,东经83.3°,北纬20°)观察到的VHF闪烁(244 MHz)。从这项研究中发现,随着太阳活动从2001年3月开始(平均Rz = 113.5)降低到赤道,等离子气泡发展的赤道层F层的阈值基准高度从405 km减少到317 km。 2005年3月(平均Rz = 24.5)。由于碰撞瑞利-泰勒不稳定性的局部线性增长率的变化,解释了阈值高度随太阳活动的降低而降低的原因,这是由于诸如反密度梯度尺度长度(L〜(- 1)),离子中性碰撞频率(v_in)和复合率(R)随太阳活动的变化而变化。

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