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Subsurface Velocity of Emerging and Decaying Active Regions

机译:新兴和衰变活动区域的地下速度

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We study the temporal variation of subsurface flows of 828 active regions and 977 quiet regions. The horizontal flows cover a range of depths from the surface to about 16 Mm and are determined by analyzing Global Oscillation Network Group high-resolution Doppler data with ring-diagram analyses. The vertical velocity component is derived from the divergence of the measured horizontal flows using mass conservation. For comparison, we analyze Michelson Doppler Imager (MDI) Dynamics Run data covering 68 active regions common to both data sets. We determine the change in unsigned magnetic flux during the disk passage of each active region using MDI magnetograms binned to the ring-diagram grid. We then sort the data by their flux change from decaying to emerging flux and divide the data into five subsets of equal size. We find that emerging flux has a faster rotation than the ambient fluid and pushes it up, as indicated by enhanced vertical velocity and faster-than-average zonal flow. After active regions are formed, downflows are established within two days of emergence in shallow layers between about 4 and 10 Mm. Emerging flux in existing active regions shows a similar scenario, where the upflows at depths greater than about 10 Mm are enhanced and the already established downflows at shallower depths are weakened. When active regions decay, the corresponding flow pattern disappears as well; the zonal flow slows down to values comparable to that of quiet regions and the upflows become weaker at deeper layers. The residual meridional velocity is mainly poleward and shows no obvious variation. The magnitude of the residual velocity, defined as the sum of the squares of the residual velocity components, increases with increasing magnetic flux and decreases with decreasing flux.
机译:我们研究了828个活动区域和977个安静区域的地下流动的时间变化。水平流覆盖了从表面到大约16 Mm的深度范围,并通过使用环图分析来分析全球振荡网络组的高分辨率多普勒数据来确定。垂直速度分量是使用质量守恒从测量的水平流的发散中得出的。为了进行比较,我们分析了涵盖两个数据集共有的68个活动区域的迈克尔逊多普勒成像仪(MDI)动态运行数据。我们使用绑定到环形图网格的MDI磁图确定每个活动区域的磁盘通过期间无符号磁通量的变化。然后,我们根据从衰减到出现的通量的通量变化对数据进行排序,然后将数据分为五个大小相等的子集。我们发现新兴的通量具有比周围流体更快的旋转速度,并且将其向上推,这可以通过增强的垂直速度和快于平均的纬向流来说明。形成有源区后,在出现的两天内,在约4至10 Mm的浅层出现了下流。现有活动区域中出现的通量显示出类似的情况,其中大于约10 Mm深度处的上升流增强,而较浅深度处已建立的下降流减弱。当活动区域衰减时,相应的流动模式也会消失;纬向流的速度减慢到与静水区相当的值,深层的向上流减弱。剩余子午线速度主要是极向,没有明显变化。剩余速度的大小定义为剩余速度分量的平方和,随着磁通量的增加而增加,而随着磁通量的减少而减小。

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