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首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Yearly variations of global plasma densities in the topside ionosphere at middle and low latitudes
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Yearly variations of global plasma densities in the topside ionosphere at middle and low latitudes

机译:每年全球等离子体密度的变化在中间和上部电离层低纬度

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In this paper, the 10-year (1996–2005) measurements of total ion density (N i ) from the Defense Meteorological Satellite Program (DMSP) spacecraft at 0930 and 2130 LT have been analyzed to investigate the yearly variations of global plasma densities in the topside ionosphere at magnetic latitudes from 60°S to 60°N. Results indicate that there are strong yearly variations in the DMSP N i at 840 km. The annual components of longitude-averaged N i dominate at most latitudes with maxima around the June solstices in the Northern Hemisphere and the December solstice in the Southern Hemisphere. In contrast, seasonal anomaly (maxima N i around the December solstice) exists in the northern equatorial zone. Moreover, the differences in N i at the two solstices are not symmetrical about the magnetic equator, being generally higher in the Southern Hemisphere than in the Northern Hemisphere. Conjugate-averaged N i is substantially greater at the December solstice than at the June solstice. This annual asymmetry is modulated by solar activity effect and has latitudinal and longitudinal structures. The longitude effects of the annual asymmetry depend on local time, being stronger in the evening sector than in the morning sector. The solstice differences and annual asymmetry are more marked with increasing solar activity. The annual asymmetry appears not only in the rising phase of the solar cycle but also in the declining phase. Thus the solar condition differences between the two solstices do not account for the N i asymmetry. The concentration of neutral oxygen [O], provided from the NRLMSIS model, shows a similar pattern of annual and hemispheric asymmetries. Moreover, effects of the HWM model neutral winds are also constituent with the change patterns of N i . Therefore, considering the principal processes in the topside ionosphere, the changes of [O] and the rates of thermospheric winds should contribute to the annual asymmetry in N i at 840-km altitude.
机译:在本文中,10年期(1996 - 2005)测量的总离子密度(N i)国防气象卫星计划(DMSP)宇宙飞船在0930年和2130年分析了LT调查每年的全球变化电离层等离子体密度在最顶上磁纬度从60°S - 60°N。表明有很强的年度变化在DMSP N我840公里。longitude-averaged N我主宰纬度与最大值在6月二至点在北半球,12月南半球的冬至。季节性异常(极大值N我在12月夏至)存在于赤道区北部。此外,N的差异在两个我二至点不对称磁赤道,在南方普遍较高比北半球的半球。Conjugate-averaged N会大得多6月在冬至日比冬至。和纬向和太阳活动影响纵向结构。一年一度的不对称依赖于当地时间晚上更强的部门早上部门。年度不对称更显著增加太阳活动。只有在太阳活动周期的上升阶段也在下降阶段。条件差异两个二至点不要占我不对称的N。氧气浓度的中性[O],提供从NRLMSIS模型,显示了类似的模式年度和半球不对称。HWM模型的影响中性风也组成与N的变化模式。因此,考虑的主要过程顶部电离层的变化[O]thermospheric风的速度为年度不对称N我在作出贡献840公里的高度。

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