Priest E R, Longcope D W
1School of Mathematics and Statistics, University of St. Andrews, Fife, KY16 9SS Scotland UK.
2Dept. of Physics, Montana State University, Bozeman, MT USA.
Sol Phys. 2017;292(1):25. doi: 10.1007/s11207-016-1049-0. Epub 2017 Jan 9.
The nature of three-dimensional reconnection when a twisted flux tube erupts during an eruptive flare or coronal mass ejection is considered. The reconnection has two phases: first of all, 3D "zipper reconnection" propagates along the initial coronal arcade, parallel to the polarity inversion line (PIL); then subsequent quasi-2D "main-phase reconnection" in the low corona around a flux rope during its eruption produces coronal loops and chromospheric ribbons that propagate away from the PIL in a direction normal to it. One scenario starts with a sheared arcade: the zipper reconnection creates a twisted flux rope of roughly one turn ( radians of twist), and then main-phase reconnection builds up the bulk of the erupting flux rope with a relatively uniform twist of a few turns. A second scenario starts with a pre-existing flux rope under the arcade. Here the zipper phase can create a core with many turns that depend on the ratio of the magnetic fluxes in the newly formed flare ribbons and the new flux rope. Main phase reconnection then adds a layer of roughly uniform twist to the twisted central core. Both phases and scenarios are modeled in a simple way that assumes the initial magnetic flux is fragmented along the PIL. The model uses conservation of magnetic helicity and flux, together with equipartition of magnetic helicity, to deduce the twist of the erupting flux rope in terms the geometry of the initial configuration. Interplanetary observations show some flux ropes have a fairly uniform twist, which could be produced when the zipper phase and any pre-existing flux rope possess small or moderate twist (up to one or two turns). Other interplanetary flux ropes have highly twisted cores (up to five turns), which could be produced when there is a pre-existing flux rope and an active zipper phase that creates substantial extra twist.
本文考虑了在爆发性耀斑或日冕物质抛射期间扭曲磁通管爆发时三维重联的性质。重联有两个阶段:首先,三维“拉链式重联”沿着初始日冕拱廊传播,平行于极性反转线(PIL);然后,在磁通绳爆发期间,低日冕中围绕磁通绳的后续准二维“主相重联”产生日冕环和色球带,它们从PIL沿垂直于它的方向传播。一种情况始于剪切拱廊:拉链式重联产生一个大约一圈扭曲( 弧度扭曲)的扭曲磁通绳,然后主相重联以几转相对均匀的扭曲形成爆发磁通绳的主体。第二种情况始于拱廊下方预先存在的磁通绳。在这里,拉链阶段可以产生一个具有许多圈的核心,这取决于新形成的耀斑带和新磁通绳中的磁通量之比。然后主相重联在扭曲的中心核心上增加一层大致均匀的扭曲。两个阶段和情况都以一种简单的方式建模,即假设初始磁通量沿PIL碎片化。该模型利用磁螺旋度和磁通量守恒,以及磁螺旋度的均分,根据初始构型的几何形状推断爆发磁通绳的扭曲。行星际观测表明,一些磁通绳具有相当均匀的扭曲,这可能是在拉链阶段和任何预先存在的磁通绳具有小或中等扭曲(最多一到两圈)时产生的。其他行星际磁通绳具有高度扭曲的核心(最多五圈),这可能是在存在预先存在的磁通绳和活跃的拉链阶段产生大量额外扭曲时产生的。