论文标题
模拟双极活动区域的冠状动力演化,以研究通量绳的形成
Simulating the Coronal Evolution of Bipolar Active Regions to Investigate the Formation of Flux Ropes
论文作者
论文摘要
使用麦凯等人的时间依赖性非线性的无线磁场方法,从其出现中模拟了20个双极活性区域(ARS)的冠状磁场演化。涵盖每个AR的整个演变的清洁光电线的时间顺序用于驱动仿真。通过手动检查,对模拟的冠状磁场与171和193的171和193 A观测值进行了比较。结果表明,有可能重现主要冠状动脉特征的演变,例如小型和大型冠状环,细丝和剪切结构,以占80%的ARS。改变边界和初始条件,以及在光球处的诸如欧姆扩散,高扩散和水平磁场注入等物理效应的添加,将观测值和模拟的冠状动脉演化之间的匹配提高了20%。模拟能够重现与ARS相关的观察到的50%的喷发爆发。与模拟中喷发开始相比,观测结果中发生的喷发之间的平均无符号时间差异约为5小时。这些模拟在捕获源自ARS内部极性反转线的所有四次爆发的爆发方面特别成功。该技术在重现起源于ARS和大规模冠状结构的爆发的发作方面不太成功。对于这些情况,必须使用全球而不是本地非线性的无线场模型。尽管该技术已经表现出了一些成功,但很难通过这种方法和模型的未来迭代来快速连续发生的爆发来解决这一问题。
The coronal magnetic field evolution of 20 bipolar active regions (ARs) is simulated from their emergence to decay using the time-dependent nonlinear force-free field method of Mackay et al. A time sequence of cleaned photospheric line-of-sight magnetograms, that covers the entire evolution of each AR, is used to drive the simulation. A comparison of the simulated coronal magnetic field with the 171 and 193 A observations obtained by the Solar Dynamics Observatory (SDO)/ Atmospheric Imaging Assembly (AIA), is made for each AR by manual inspection. The results show that it is possible to reproduce the evolution of the main coronal features such as small- and large-scale coronal loops, filaments and sheared structures for 80% of the ARs. Varying the boundary and initial conditions, along with the addition of physical effects such as Ohmic diffusion, hyperdiffusion and a horizontal magnetic field injection at the photosphere, improves the match between the observations and simulated coronal evolution by 20%. The simulations were able to reproduce the build-up to eruption for 50% of the observed eruptions associated with the ARs. The mean unsigned time difference between the eruptions occurring in the observations compared to the time of eruption onset in the simulations was found to be ~5 hrs. The simulations were particularly successful in capturing the build-up to eruption for all four eruptions that originated from the internal polarity inversion line of the ARs. The technique was less successful in reproducing the onset of eruptions that originated from the periphery of ARs and large-scale coronal structures. For these cases global, rather than local, nonlinear force-free field models must be used. While the technique has shown some success, eruptions that occur in quick succession are difficult to reproduce by this method and future iterations of the model need to address this.