首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Jupiter's Dark Polar Region as Observed by the Hubble Space Telescope During the Juno Approach Phase
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Jupiter's Dark Polar Region as Observed by the Hubble Space Telescope During the Juno Approach Phase

机译:Jupiter的暗极区域,由哈莫接近阶段的哈勃太空望远镜观察

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摘要

We present an analysis of Jupiter's dark polar region, previously described as a crescent-shaped region devoid of emission along the dawnside poleward of the main oval. Using ultraviolet images obtained by the Hubble Space Telescope between days of year 137 and 176, coupled with interplanetary data captured during the approach phase of the NASA Juno spacecraft, we examine the morphology and variability of the dark polar region and the influence of solar wind conditions on the region.We find that the dark polar region is more variable than previously thought and in particular shows significant variability during compressions of the magnetosphere by the solar wind. Duskward extensions of the dark polar region through the noon sector are often observed during periods of deep rarefaction in the solar wind, while a larger dark polar region width is observed nearer to local noon under solar wind compression. Intensity distributions of the dark polar region reveal a greater probability of lower emission intensity during deep rarefactions. Calculation of the magnetic flux associated with the dark polar region returns lower flux values than previous estimates of the total open flux at Jupiter. This may suggest that either the dark polar region does not account for the entirety of the open flux region, or the magnetotail is not composed of only open flux, as previously suggested.
机译:我们对木星的暗极性区域进行了分析,以前描述为沿着主椭圆形的垂直垂直发射的新月形区域。在137和176年之间使用哈勃空间望远镜的紫外线图像,与在美国宇航局朱诺航天器的接近阶段捕获的行星数据,我们研究了黑暗极地区域的形态和可变性以及太阳风条件的影响在该地区。我们发现暗极性区域比以前认为暗极性区域更具变量,特别是在太阳风中磁性层的按压期间显着差异。在太阳风中的深度稀疏期间,通常观察到暗极性区域的暗极区域的延伸延伸,而在太阳风压缩下,观察到更大的暗极区域宽度较较大的暗极性区域宽度。暗极性区域的强度分布揭示了在深稀疏期间较低发射强度的更大概率。与暗极性区域相关联的磁通量的计算返回比JUPITER的总开放通量的先前估计值下降的磁通值。这可能表明,如前所述,暗极地区域不考虑整个开放通量区域,或者磁靶不由开放的通量组成。

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