太阳活跃区域日冕加热过程中的大尺度电流

Pub Date : 2023-07-31 DOI:10.1007/s10511-023-09786-y
Yu.A. Fursyak
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摘要

本文提出了研究在太阳日冕加热过程中在太阳大气上层传播的大尺度电流的作用的问题。为了探测和计算大尺度电流的大小,利用太阳动力学观测台(SDO)上的日震磁成像仪(HMI)提供的光球磁场矢量分量分布数据。大气成像组件(AIA/SDO)提供的太阳日冕在紫外线辐射通道131、171、193和211 Å的日冕照片被用来估计活跃区域(ARs)以上日冕的温度。本文研究了太阳耀斑活动程度不同的9个区域的大尺度电流和平均温度的动态变化,并绘制了太阳耀斑活动程度不同的日冕温度空间分布图。实验结果如下:1.实验结果如下:由于大规模电流的欧姆耗散,日冕物质的加热是在固定状态下进行的。2. 在太阳耀斑期间,AR上方日冕的平均温度升高到\(<\overline{\mathrm{log}T }>=6.3-6.5\) (2.0-3.2 MK),这不仅是由大规模电流对日冕结构的加热引起的,而且是由日冕高度的其他过程引起的。3.在NOAA 11899和12494区域观测到日冕平均温度降至\(<\overline{\mathrm{log}T }>=5.7\) (0.5-0.6 MK),同时大尺度电流值降至零。这些观测结果表明,通过电流的欧姆耗散加热电晕的机制在大电流的零值(在计算误差范围内)被关闭。4. 在NOAA 12192和12371区域,在构建耀斑事件外日冕温度分布图时,在耀斑事件外观测到温度≥10 MK的热结构,这些热结构似乎标志着日冕高度处大范围电流通道的位置。对于NOAA 12192区域,2016年进行的数值模拟证实了这一假设。
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Large-Scale Electric Currents in Coronal Heating Processes above Active Regions on the Sun

This paper poses the problem of studying the role of large-scale electric currents propagating in the upper layers of the solar atmosphere in processes of coronal heating of the sun. For detecting and calculating the magnitude of the large-scale electric current, data on the distribution of the components of the magnetic field vector in the photosphere provided by the Helioseismic and Magnetic Imager (HMI) on board the Solar Dynamics Observatory (SDO) were used. Photoheliograms of the sun’s corona in the ultraviolet radiation channels at 131, 171, 193, and 211 Å provided by the Atmospheric Imaging Assembly (AIA/SDO) were used to estimate the temperature in the corona above active regions (ARs). The dynamics of the large-scale current and the average temperature in 9 regions with different levels of flare activity of the corona above the ARs have been studied and charts of the spatial distribution of the temperature in the corona above the ARs have been constructed. The following results have been obtained: 1. Heating of the coronal matter owing to ohmic dissipation of large-scale electric currents proceeds in a stationary regime. 2. The increase in the average temperature in the corona above an AR during solar flares to \(<\overline{\mathrm{log}T }>=6.3-6.5\) (2.0-3.2 MK) is caused, not only by heating of coronal structures by large-scale electric currents, but also by other processes at coronal elevations. 3. For the NOAA 11899 and 12494 regions a reduction in the average temperature of the corona to \(<\overline{\mathrm{log}T }>=5.7\) (0.5-0.6 MK) was observed with a simultaneous drop in the values of the large-scale electric current to zero. These observations indicate that the mechanism for heating of the corona by ohmic dissipation of electric currents is shut off at zero values (within the computational errors) of the large-scale electric current. 4. In the NOAA regions 12192 and 12371, when constructing charts of the temperature distribution in the corona outside flare events, hot structures with temperatures ≥ 10 MK were observed outside the flare events which appear to mark the location of the channel of a large-scale electric current at coronal elevations. For the NOAA region 12192 this assumption is confirmed by a numerical simulation carried out in 2016.

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