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Planetary Distribution of Auroral Precipitation and Its Relation to the Zones of Auroral Luminosity

机译:极光降水的行星分布及其与极光亮度区的关系

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Boundaries of different auroral precipitation have been determined based on data of the DMSP F6 and F7 satellites. The boundaries of auroral precipitation on the day and night sides of the Earth have been joined proceeding from the new terminology of electron precipitation [Starkov et al., 2002]. The planetary pattern of precipitation at different levels of magnetic activity has been constructed. It has been indicated that the auroral oval precipitation (AOP) spatially coincides with the auroral oval. The zones of diffuse precipitation (diffuse auroral zone. DAZ) and diffuse auroral luminosity coincide at low and moderate magnetic activity. At high magnetic activity, the low-latitude auroral edge is sometimes observed equatorward of the corresponding precipitation boundary. The dynamics of the narrow belt of soft diffuse precipitation (SDP), located poleward of the auroral oval, has been studied. It has been indicated that, at low magnetic activity, this precipitation surrounds the AOP one in the form of a belt with a width of ~2°in latitude. With increasing magnetic activity, this belt becomes narrower and disappears on the nightside at |AL| > 400 nT. The polar cap boundaries have been determined. It has been indicated that the polar cap area linearly increases with increasing magnetic activity. At high magnetic activity (|AL| > 400 nT), the polar cap area is twice as large as under quiet conditions. The growth of magnetic disturbance results in a synchronous widening and simultaneous equatorward shift of the zones of auroral luminosity and precipitation.
机译:已根据DMSP F6和F7卫星的数据确定了极光降水的边界。从电子降水的新术语出发,已经将地球白天和黑夜的极光降水的边界结合了起来[Starkov et al。,2002]。构造了不同磁性活动水平的降水行星模式。已经表明,极光椭圆形降水(AOP)在空间上与极光椭圆形重合。在低和中等磁活动下,弥散的降水区(弥散的极光区。DAZ)和弥散的极光亮度重合。在高磁性活动下,有时会观察到低纬度的极光边缘在相应的降水边界的赤道线上。研究了极光椭圆极处的软弥散降水(SDP)狭窄带的动力学。已经表明,在低磁活度下,这种沉淀以带状形式围绕AOP,其宽度为纬度〜2°。随着磁活动的增加,该带变窄并在夜间在| AL |消失。 > 400 nT。极帽边界已确定。已经表明,极帽面积随着磁活动的增加而线性增加。在高磁性活动(| AL |> 400 nT)下,极帽面积是安静条件下的两倍。磁干扰的增长导致极光亮度和降水区域同步加宽和同时向赤道移动。

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