Magnetic helicity and energy budget around large confined and eruptive solar flares.

M. Gupta, J. Thalmann, A. Veronig
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引用次数: 15

Abstract

We investigate the coronal magnetic energy and helicity budgets of ten solar ARs, around the times of large flares. In particular, we are interested in a possible relation of the derived quantities to the particular type of the flares that the AR produces, i.e., whether they are associated with a CME or they are confined. Using an optimization approach, we employ time series of 3D nonlinear force-free magnetic field models of ten ARs, covering a time span of several hours around the time of occurrence of large solar flares (GOES class M1.0 and larger). We subsequently compute the 3D magnetic vector potentials associated to the model 3D coronal magnetic field using a finite-volume method. This allows us to correspondingly compute the coronal magnetic energy and helicity budgets, as well as related (intensive) quantities such as the relative contribution of free magnetic energy, $E_{\mathrm{F}}/{E}$ (energy ratio), the fraction of non-potential (current-carrying) helicity, $|H_{\mathrm{J}}|/|{H_{V}}|$ (helicity ratio), and the normalized current-carrying helicity, $|H_{\mathrm{J}}|/{\phi^{\prime}}^{2}$. The total energy and helicity budgets of flare-productive ARs (extensive parameters) cover a broad range of magnitudes, with no obvious relation to the eruptive potential of the individual ARs, i.e., whether or not a CME is produced in association with the flare. The intensive eruptivity proxies, $E_{\mathrm{F}}/{E}$ and $|H_{\mathrm{J}}|/|{H_{V}}|$, and $|H_{\mathrm{J}}|/{\phi^{\prime}}^{2}$, however, seem to be distinctly different for ARs that produced CME-associated large flares compared to those which produced confined flares. For the majority of ARs in our sample, we are able to identify characteristic pre-flare magnitudes of the intensive quantities, clearly associated to subsequent CME-productivity.
大的受限的和喷发的太阳耀斑周围的磁螺旋度和能量收支。
我们研究了10个太阳ARs在大耀斑发生前后的日冕磁能和螺旋度收支。我们特别感兴趣的是,导出的量与AR产生的特定类型的耀斑之间的可能关系,即它们是否与CME有关还是受到限制。利用优化方法,我们采用了10个ar的三维非线性无力磁场模型的时间序列,覆盖了大型太阳耀斑(GOES M1.0级及以上)发生时间前后几个小时的时间跨度。随后,我们使用有限体积法计算了与模型三维日冕磁场相关的三维磁矢量势。这允许我们相应地计算日冕磁能和螺旋度预算,以及相关的(密集)量,如自由磁能的相对贡献,$E_{\ mathm {F}}/{E}$(能量比),非电位(载流)螺旋度的分数,$|H_{\ mathm {J}}|/|{H_{V}}|$(螺旋比),和归一化载流螺旋度,$|H_{\ mathm {J}}|/{\phi^{\prime}}^{2}$。产生耀斑的太阳太阳的总能量和螺旋度预算(广泛的参数)覆盖了很宽的量级范围,与单个太阳太阳太阳的爆发潜力没有明显的关系,也就是说,CME是否与耀斑有关。然而,对于产生cme相关的大耀斑的ARs而言,与产生受限耀斑的ARs相比,密集喷发代理$E_{\mathrm{F}}/{E}$和$|H_{\mathrm{J}}|/|{H_{V}}}和$|H_{\mathrm{J}}|/{\phi^{\prime}}^{2}$似乎有明显的不同。对于我们样本中的大多数ar,我们能够识别出耀斑前密集数量的特征大小,这与随后的日冕物质抛射生产力明显相关。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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