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Findings concerning the positions of substorm onsets with auroral images from the Polar spacecraft

机译:通过极地飞船的极光图像发现亚暴发作位置的发现

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High-resolution global images of Earth's auroras in the visible emissions of atomic oxygen at 557.7 nm with a camera on board the Polar spacecraft were used to determine the magnetic latitude of the auroral are which brightens at the onset of a substorm. Six events were analyzed: an intensification and an onset on December 17, 1997, three substorms on January 6, 1998, and a substorm on March 1, 1999. The Tsyganenko [1989] model for the global magnetic field was used to map the field lines threading the center of the auroral are to equatorial distances. During the period of relative magnetic quiescence on December 17 the equatorial distances were similar to 9 R-E. During the magnetically disturbed periods of January 6 and March 1 the magnetic field lines for the auroral onset brightenings were mapped to equatorial distances in the range of 5-7 R-E, and thus in the region of the extraterrestrial ring current. The equatorial position of the field lines was independently verified for the substorm on March 1 by observing the atmospheric footprint of proton precipitation from the ring current. This footprint was seen in the emissions of atomic hydrogen at 656.3 nm. The onset are was located near the earthward edge of the ring current at magnetic shell parameter L = 4 R-E and within 1 R-E of the equatorial position computed with the global magnetic field model. The equatorial distance of the elusive substorm onset is important in establishing plasma parameters for quantitative evaluation of candidate mechanisms for the explosive instability that initiates substorms. [References: 45]
机译:使用Polar太空飞船上的摄像头,在557.7 nm的可见氧原子可见发射中,高分辨率的地球极光全球图像被用于确定极光的磁纬度,这在亚暴爆发时会变亮。分析了六个事件:1997年12月17日发生了一次强化和一次爆发,​​1998年1月6日发生了3次亚暴,1999年3月1日发生了一次亚暴。使用了全球磁场的Tsyganenko [1989]模型来绘制磁场穿过极光中心的线是赤道距离。在12月17日的相对磁性静止期间,赤道距离与9 R-E相似。在1月6日和3月1日的磁干扰期间,极光开始增亮的磁力线映射到赤道距离为5-7 R-E,因此在地外环流区域。通过观察环流中质子的大气足迹,3月1日针对亚暴对场线的赤道位置进行了独立验证。在656.3 nm的氢原子发射中可以看到这一足迹。起始点位于磁壳参数L = 4 R-E时,位于环电流的大地边缘附近,并且位于用整体磁场模型计算的赤道位置的1 R-E内。难以捉摸的亚暴爆发的赤道距离对于建立等离子参数以定量评估引发亚暴的爆炸性不稳定的候选机制非常重要。 [参考:45]

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