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首页> 外文期刊>Solar Physics >The Flare-Energy Distributions Generated by Kink-Unstable Ensembles of Zero-Net-Current Coronal Loops
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The Flare-Energy Distributions Generated by Kink-Unstable Ensembles of Zero-Net-Current Coronal Loops

机译:零净电流冠状环的扭结不稳定集合产生的耀斑能量分布

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It has been proposed that the million-degree temperature of the corona is due to the combined effect of barely detectable energy releases, called nanoflares, that occur throughout the solar atmosphere. Unfortunately, the nanoflare density and brightness implied by this hypothesis means that conclusive verification is beyond present observational abilities. Nevertheless, we investigate the plausibility of the nanoflare hypothesis by constructing a magnetohydrodynamic (MHD) model that can derive the energy of a nanoflare from the nature of an ideal kink instability. The set of energy-releasing instabilities is captured by an instability threshold for linear kink modes. Each point on the threshold is associated with a unique energy release; thus we can predict a distribution of nanoflare energies. When the linear instability threshold is crossed, the instability enters a nonlinear phase as it is driven by current sheet reconnection. As the ensuing flare erupts and declines, the field transitions to a lower energy state, which is modelled by relaxation theory; i.e., helicity is conserved and the ratio of current to field becomes invariant within the loop. We apply the model so that all the loops within an ensemble achieve instability followed by energy-releasing relaxation. The result is a nanoflare energy distribution. Furthermore, we produce different distributions by varying the loop aspect ratio, the nature of the path to instability taken by each loop and also the level of radial expansion that may accompany loop relaxation. The heating rate obtained is just sufficient for coronal heating. In addition, we also show that kink instability cannot be associated with a critical magnetic twist value for every point along the instability threshold.
机译:已经提出,电晕的百万度温度是由于在整个太阳大气中几乎无法检测到的被称为纳米耀斑的能量释放的综合作用所致。不幸的是,该假设所隐含的纳米耀斑密度和亮度意味着结论性验证超出了当前的观察能力。尽管如此,我们通过构建磁流体动力学(MHD)模型来研究纳米耀斑假说的合理性,该模型可以从理想扭结不稳定性的性质中得出纳米耀斑的能量。能量释放不稳定性的集合由线性扭折模式的不稳定性阈值捕获。阈值上的每个点都与唯一的能量释放相关。因此我们可以预测纳米火炬能量的分布。当超过线性不稳定性阈值时,不稳定性进入非线性阶段,这是由电流表重新连接驱动的。随着随之而来的耀斑的爆发和下降,磁场转变为能量较低的状态,这是由弛豫理论建模的。即,螺旋度被保留,并且电流与磁场的比率在环路内变得不变。我们应用该模型,以使集合内的所有环路均达到不稳定性,然后释放能量。结果是纳米火炬能量分布。此外,我们通过改变环的长宽比,每个环的不稳定性路径的性质以及可能伴随环松弛的径向扩展水平来产生不同的分布。所获得的加热速率刚好足以进行冠状加热。此外,我们还表明,对于沿不稳定性阈值的每个点,扭结不稳定性都无法与临界磁扭曲值相关联。

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