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首页> 外文期刊>Solar Physics >Sequential Coronal Mass Ejections from AR8038 in May 1997
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Sequential Coronal Mass Ejections from AR8038 in May 1997

机译:1997年5月从AR8038逐次冠状大体射出

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Three homologous coronal mass ejections (CMEs) occurred on 5, 12 and 16 May 1997 from the single magnetic polarity inversion line (PIL) of AR8038. The three events together provide STEREO-like quadrature views of the 12 May 1997 CME and EIT double dimming. The recurrent CMEs with the nearly identical post-CME potential state and the ‘sigmoid to arcade to sigmoid’ transformations indicate a repeatable store – release – restore process of the free energy. How was the free magnetic energy re-introduced to the potential state corona after each release in this decaying active region? Making use of the known time interval bounded by the adjacent homologous CMEs, we made the following measures. The unsigned magnetic flux of AR8038, ΦAR, decreased by approximately 18% during 66 h, while the unsigned flux, ΦPIL, in a Gaussian-weighted PIL-region containing the flare site increased by about 50% during 36 hrs prior to the C1.3 flare on 12 May 1997. The significant increase of ΦPIL demonstrates the magnetic gradient increase and the build-up of free energy in the PIL-region during the time leading to the eruption. Fourier local correlation tracking (FLCT) flow speed in AR8038 ranges from 0 to 292.8 m s−1 with a mean value of 63.2 m s−1. The flow field contains a persistent converging flow towards the flaring PIL and an effective shear flow distributed in the AR. Minor angular motions were found. An integrated proxy Poynting flux S h estimates the energy input to the corona to be on the order of 1.15×1032 erg during the 66 hrs before the C1.3 flare. It suggests that sufficient energy for a flare/CME can be introduced to the corona on the order of several days by the flows deduced from photospheric magnetic field motions in this small decaying active region.
机译:1997年5月5日,12日和16日,AR8038的单条极性反​​转线(PIL)发生了三个同源冠状物质抛射(CME)。这三个事件共同提供了1997年5月12日CME和EIT双重调光的STEREO式正交视图。循环CME的后CME势态几乎相同,并且从“ S型弧线到S型弧线”的转换表明自由能的可重复存储-释放-恢复过程。在此衰减的活性区域中每次释放后,如何将自由磁能重新引入电势态电晕?利用相邻同源CME界定的已知时间间隔,我们采取了以下措施。在高斯加权的PIL区域中,AR8038的无符号磁通量Φ AR 在66小时内下降了约18%,而无符号磁通量Φ PIL 在1997年5月12日C1.3耀斑爆发之前的36个小时内,耀斑的位置增加了约50%。Φ PIL 的显着增加证明了磁梯度的增加和自由能的积累。导致喷发期间的PIL区域。 AR8038中的傅立叶局部相关跟踪(FLCT)流速范围为0到292.8 m s -1 ,平均值为63.2 m s -1 。流场包含朝向扩口PIL的持续会聚流和分布在AR中的有效剪切流。发现较小的角度运动。集成的代理珀因廷通量S h 估计,在C1.3爆发前的66个小时内,输入电晕的能量约为1.15×10 32 erg。这表明通过在这个小的衰减活性区域中从光球磁场运动推导出的流量,可以在几天的数量级将火炬/ CME的足够能量引入电晕。

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