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首页> 外文期刊>The Astrophysical Journal. Letters >KINEMATICS AND FINE STRUCTURE OF AN UNWINDING POLAR JET OBSERVED BY THE SOLAR DYNAMIC OBSERVATORY/ATMOSPHERIC IMAGING ASSEMBLY
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KINEMATICS AND FINE STRUCTURE OF AN UNWINDING POLAR JET OBSERVED BY THE SOLAR DYNAMIC OBSERVATORY/ATMOSPHERIC IMAGING ASSEMBLY

机译:太阳动力观测/大气成象组件观测到的解旋极地射流的运动学和精细结构

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摘要

We present an observational study of the kinematics and fine structure of an unwinding polar jet, with high temporal and spatial observations taken by the Atmospheric Imaging Assembly on board the Solar Dynamic Observatory and the Solar Magnetic Activity Research Telescope. During the rising period, the shape of the jet resembled a cylinder with helical structures on the surface, while the mass of the jet was mainly distributed on the cylinder’s shell. In the radial direction, the jet expanded successively at its western side and underwent three distinct phases: the gradually expanding phase, the fast expanding phase, and the steady phase. Each phase lasted for about 12 minutes. The angular speed of the unwinding motion of the jet and the twist transferred into the outer corona during the eruption are estimated to be 11.1 × 10~(-3) rad s~(-1) (period = 564 s) and 1.17–2.55 turns (or 2.34–5.1π), respectively. On the other hand, by calculating the azimuthal component of the magnetic field in the jet and comparing the free energy stored in the non-potential magnetic field with the jet’s total energy, we find that the non-potential magnetic field in the jet is enough to supply the energy for the ejection. These new observational results strongly support the scenario that the jets are driven by the magnetic twist, which is stored in the twisted closed field of a small bipole, and released through magnetic reconnection between the bipole and its ambient open field.
机译:我们目前正在对退绕的极地喷气的运动学和精细结构进行观测研究,并由太阳动力天文台和太阳磁活动研究望远镜上的大气成像组件进行高时空观测。在上升期间,喷流的形状类似于表面上具有螺旋结构的圆柱体,而喷流的质量主要分布在圆柱体的壳体上。在径向方向上,射流在其西侧连续膨胀,并经历了三个不同的阶段:逐渐膨胀阶段,快速膨胀阶段和稳定阶段。每个阶段持续约12分钟。喷流的退绕运动和喷发过程中传递到外日冕的扭曲的角速度估计为11.1×10〜(-3)rad s〜(-1)(周期= 564 s)和1.17–2.55转(或2.34–5.1π)。另一方面,通过计算射流中磁场的方位分量,并将存储在非势磁场中的自由能与射流的总能量进行比较,我们发现射流中的非势磁场就足够了为喷射提供能量。这些新的观测结果有力地支持了射流由磁扭曲驱动的情况,磁扭曲被存储在小双极子的扭曲封闭场中,并通过双极子与其周围的开放场之间的磁重连接而释放。

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