从南极测得的白天热层风与 IMF By 的关系

Ying Zou, Cheng Sheng, Mark Conde, Xueling Shi, William A. Bristow, Yen-Jung Joanne Wu
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摘要

夜间热层上部的风经常被观测到模仿极地纬度的电离层等离子体对流,白天的风是否也是如此仍不清楚。日侧扇区受到太阳辐照度形成的巨大温度梯度的影响,它还包含尖顶,尖顶是波因廷通量的热点,也是软粒子降水最强的区域。我们利用位于南极的扫描多普勒成像仪(SDI)对昼间风进行了研究,并调查了它们在稳定的正负IMF By条件下的分布情况。结果表明,昼间风与等离子体对流存在显著差异。在负的 IMF By 条件下,风的流动方向与等离子带相同,但在极光带有最强的经向分量。因此,极光区内的风比等离子体对流更偏向极地,而在极冠区则更偏向西方。在正 IMF 条件下,某些区域的风会逆等离子体的方向流动。例如,在极冠,尽管等离子体对流向东,风却向西流动,与等离子体对流形成一个大角度。结果表明,离子阻力可能不是白天风的最主要作用力。虽然利用数据集无法确定各种作用力的重要性,但我们推测尖顶加热时的压力梯度力是一个重要的作用力。
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Dependence of daytime thermospheric winds on IMF By as measured from south pole
Winds in the nighttime upper thermosphere are often observed to mimic the ionospheric plasma convection at polar latitudes, and whether the same is true for the daytime winds remains unclear. The dayside sector is subject to large temperature gradient set up by solar irradiance and it also contains the cusp, which is a hotspot of Poynting flux and a region with the strongest soft particle precipitation. We examine daytime winds using a Scanning Doppler Imager (SDI) located at the South Pole, and investigate their distribution under steadily positive and negative IMF By conditions. The results show that daytime winds exhibit significant differences from the plasma convection. Under negative IMF By conditions, winds flow in the same direction as the plasma zonally, but have a meridional component that is strongest in the auroral zone. As a result, winds are more poleward-directed than the plasma convection within the auroral zone, and more westward-directed in the polar cap. Under positive IMF By conditions, winds can flow zonally against the plasma in certain regions. For instance, they flow westward in the polar cap despite the eastward plasma convection there, forming a large angle relative to the plasma convection. The results indicate that ion drag may not be the most dominant force for daytime winds. Although the importance of various forcing terms cannot be resolved with the utilized dataset, we speculate that the pressure gradient force in the presence of cusp heating serves as one important contributor.
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