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Solar Flux Emergence Simulations

机译:太阳通量出现模拟

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We simulate the rise through the upper convection zone and emergence through the solar surface of initially uniform, untwisted, horizontal magnetic flux, with the same entropy as the nonmagnetic plasma, that is advected into a domain 48 Mm wide by 20 Mm deep. The magnetic field is advected upward by the diverging upflows and pulled down in the downdrafts, which produces a hierarchy of loop-like structures of increasingly smaller scale as the surface is approached. There are significant differences between the behavior of fields of 10 kG and 20 or 40 kG strength at 20 Mm depth. The 10 kG fields have little effect on the convective flows and show small magnetic-buoyancy effects, reaching the surface in the typical fluid rise time from 20 Mm depth of 32 hours. 20 and 40 kG fields significantly modify the convective flows, leading to long, thin cells of ascending fluid aligned with the magnetic field and their magnetic buoyancy makes them rise to the surface faster than the fluid rise time. The 20 kG field produces a large-scale magnetic loop that as it emerges through the surface leads to the formation of a bipolar, pore-like structure.
机译:我们模拟了通过上部对流区的上升,并通过初始均匀,未扭曲的水平磁通量的太阳表面出现,其熵与非磁性等离子体相同,并被平流到48 Mm宽,20 Mm深的磁畴中。磁场由于发散的向上流动而向上平移,并在向下的气流中被拉低,随着接近表面,这会产生越来越小的比例的环状结构的层次结构。在20 Mm深度下,强度为10 kG和强度为20或40 kG的场的行为之间存在显着差异。 10 kG磁场对对流几乎没有影响,磁浮力影响也很小,在典型的流体上升时间内从20 Mm深度(32小时)到达表面。 20 kG和40 kG场显着改变了对流,导致上升流体的细长的细长单元与磁场对齐,它们的磁性浮力使它们上升到表面的速度快于流体上升时间。 20 kG磁场会产生大规模的磁环,当其通过表面出现时,会导致形成双极性的孔状结构。

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