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首页> 外文期刊>The Astrophysical journal >THE PECULIAR BEHAVIOR OF THE LARGE-SCALE COMPONENTS OF THE SOLAR MAGNETIC FIELD AS A RESULT OF ROSSBY VORTEX EXCITATION BENEATH THE CONVECTION ZONE
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THE PECULIAR BEHAVIOR OF THE LARGE-SCALE COMPONENTS OF THE SOLAR MAGNETIC FIELD AS A RESULT OF ROSSBY VORTEX EXCITATION BENEATH THE CONVECTION ZONE

机译:对流区下方罗斯比涡旋激发的结果是,太阳磁场大分量的特有行为

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摘要

To interpret the dynamical features of large-scale magnetic fields, Rossby vortices are considered. Rossby vortices are assumed to be excited and sustained within a thin layer beneath the convection zone as a result of heating from the solar interior and deformation of the covection zone lower boundary. Numerical calculations show that a Rossby cyclone generates a large-scale magnetic structure, whose horizontal size compares with the solar radius. The distribution of the vertical component of the magnetic field bears a resemblance in this case to the cloud distribution in the cyclones that are observed in the Earth's atmosphere. A magnetic field with the sign of trailing polarity flux of the local bipolar magnetic regions and a field with the sign of leading polarity are generated, respectively, at the center of the Rossby cyclone and at the periphery. The drift of the cyclone toward the Sun's pole, caused by the Rossby wave emission, leads to a corresponding drift of the large-scale magnetic structure. Longitudinally averaged magnetic field distribution also drifts poleward and has a form of " double surge." The leading polarity is the first to reach the pole. The rotation of the first Fourier components of magnetic field calculated for the low- and midlatitude belts resembles in this case the real picture during the threefold polar field reversal in solar activity cycle. Rossby cyclones are used also to simulate some other situations on the Sun when, according to observational data, there are weak drifts of the longitudinally averaged component and corotation of the first Fourier components of the low- and midlatitude belts.
机译:为了解释大范围磁场的动力学特征,考虑了罗斯比涡旋。由于太阳内部的加热和对流区下边界的变形,Rossby涡被认为在对流区下方的薄层内被激发和维持。数值计算表明,罗斯比旋风产生了一个大型的磁性结构,其水平尺寸与太阳半径相比较。在这种情况下,磁场垂直分量的分布与在地球大气中观察到的旋风中的云分布相似。在罗斯比旋风分离器的中心和外围分别产生了带有局部双极磁性区域的尾随极性通量的符号的磁场和带有超前极性的极性的场。由罗斯比波发射引起的旋风向太阳极的漂移导致大型磁性结构的相应漂移。纵向平均磁场分布也向极点漂移并具有“双重浪涌”形式。引导极性是第一个到达极点的极性。在这种情况下,为低纬度和中纬度带计算的磁场的第一傅立叶分量的旋转类似于太阳活动周期中三倍极性场反转期间的真实情况。当根据观测数据,低纬度和中纬度带的纵向平均分量漂移较小且第一傅里叶分量同向旋转时,罗斯比气旋也可用于模拟太阳上的其他情况。

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