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Influence of solar flare's location and heliospheric current sheet on the associated shock's arrival at Earth

机译:太阳耀斑的位置和影响日球电流片的关联冲击到达地球

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We study the source locations of 130 solar flare-type II radio burst events with the associated interplanetary shocks observed by L1 spacecraft (type A events) and 217 flare-type II events without such shocks observed at L1 (type B events) during February 1997–August 2002. In particular, we investigate the relative positions between the flare sources, the heliospheric current sheet (HCS), and the Earth. We found the following results: (1) Solar flares are usually distributed within [S30°, N30°] in heliographic latitude and [S30°, N30°] × [E10°, W30°] is the predominant source region on the solar disk that includes the majority of geoeffective solar flares. (2) The shocks with the associated flares located near the HCS would have a lower probably of reaching the Earth. For the Earth-encountered shocks, their initial speeds are distinctly higher when their associated flares are located near the HCS. (3) The angular distance from the flare source to the Earth (defined as Ψ below) also contributes to the probability of the associated shock being observed at the Earth. The shock arrival probability decreases with the increment of Ψ and the mean initial shock speed increases with Ψ for those Earth-encountered shocks. (4) The so-called “same-opposite side effect” of the HCS is confirmed to exist. That is, the shocks whose associated flares are located on the same side of the HCS as the Earth (called as “same side events”) have a greater chance of reaching the Earth than those shocks with their associated flares on the opposite side (“opposite side events”). Here for the first time, a comprehensive sample of solar transient events of both arriving and nonarriving ones (at Earth) is used to testify to the same-opposite side effect. These results would be valuable in understanding the solar-terrestrial relations, and helpful for space weather prediction.
机译:我们研究130个太阳能的来源位置flare-type II无线电破裂事件的有关星际冲击L1观察到航天器(输入一个事件)和217年flare-type II没有这样的事件冲击观察到L1 (B型事件)在1997年2月- 2002年8月。特别地,我们调查的相对位置之间的耀斑来源,日球当前表(高碳钢)和地球。以下结果:(1)太阳耀斑通常分布在[S30°,N30°)在日面纬度和[S30°,N30°)×(E10°,W30°)是太阳能磁盘上的主要源区包括大多数geoeffective太阳能耀斑。高碳钢附近可能会更低到达地球。冲击,他们的初始速度明显当它们相关的耀斑位于更高在高碳钢附近。耀斑源地球(如下Ψ定义)同样会引起的概率相关冲击地球被观察到。冲击到达概率随Ψ增量和意味着初始冲击速度随ΨEarth-encountered冲击。高碳钢的效应”是证实存在。是,太阳耀斑是相关的冲击的位于同一侧高碳钢的地球相同(称为“事件”)有一个更大的到达地球的机会比冲击与它们相关的耀斑对面(“对面事件”)。太阳能瞬态的时间,一个全面的样本事件到达和nonarriving (same-opposite地球)用来作证副作用。日地关系,理解和对空间天气预报。

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