Spatial and Temporal Scales of Coronal Magnetic Restructuring in the Development of Coronal Mass Ejections
Spatial and Temporal Scales of Coronal Magnetic Restructuring in the Development of Coronal Mass Ejections
复制标题
DOI:
10.1007/s11207-006-0181-7
复制
发表时间:
2006-12
期刊:
影响因子:
2.8
通讯作者:
Y. Wen;Jingxiu Wang;D. Maia;Yuzong Zhang;Hui Zhao;Guiping Zhou
中科院分区:
文献类型:
--
作者:
Y. Wen;Jingxiu Wang;D. Maia;Yuzong Zhang;Hui Zhao;Guiping Zhou
It has been commonly accepted that coronal mass ejections (CMEs) result from the restructuring or reconfiguring of large-scale coronal magnetic fields. In this paper, we analyzed four CME events using Nançay Radioheliograph (NRH) images and the experiments onboard the Solar and Heliospheric Observatory (SOHO) spacecraft to understand the coronal restructuring leading to CME initiation. We investigated the onset, duration, and position of the radio emissions in relation to EUV dimming and the inferred CME onset.It has been identified that the early CME development on the solar disk is characterized by a series of distinct radio bursts. These nonthermal radio sources appeared in phase with coronal dimming shown by SOHO-EIT images and are located within the EUV dimming or ongoing dimming regions. Three time scales are identified: the duration, the separation of individual radio bursts, and the overall time scale of all of the nonthermal sources. They fall in the ranges of approximately tens of seconds to three minutes, one to three minutes, and 15 – 20 minutes, respectively. The individual radio emission seems to shift and expand at the speed of the fast magnetoacoustic waves in the corona; while the nonthermal radio emissions as a whole appear episodically to correspond to the successive coronal restructuring. If we define the triggering speed by dividing the overall spatial scale by the temporal scale of all the radio bursts, then the triggering speed falls in the range of 300 – 400 km s−1. This implies that the general process of coronal restructuring and reconfiguring takes place at a speed slower than either the Alvfenic or acoustic speed in the corona. This is a type of speed of “topology waves,”i.e., the speed of successive topology changes from closed to open field configuration.