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哈雷彗星主尾流的研究
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作者 赵海斌 胡中为 +1 位作者 王建中 侯振宇 《天文学报》 CSCD 北大核心 2002年第1期66-74,共9页
哈雷彗星在日彗距较大时出现长而直的主彗尾(尾流);这是很有趣的.尾流一般是指等离子体尾流;但是,当地球接近彗星轨道面时;尘埃尾流可能叠加到主彗尾上.在一般感光波段宽的彗星底片上很难区分这两种尾流.本文选取哈雷彗星在不... 哈雷彗星在日彗距较大时出现长而直的主彗尾(尾流);这是很有趣的.尾流一般是指等离子体尾流;但是,当地球接近彗星轨道面时;尘埃尾流可能叠加到主彗尾上.在一般感光波段宽的彗星底片上很难区分这两种尾流.本文选取哈雷彗星在不同日彗距的5条主尾流;作了光度测量和比较分析.得出沿各尾轴及其垂直方向几个截面的亮度分布、亮度半极大全宽、尾轴的视风差角和真风差角及彗尾长度.在所分析的蓝敏底片上,过近日点前的2个尾流肯定是等离子体尾流,而5个尾流的相似性以及其他证据说明它们主要都是等离子体尾流。 展开更多
关键词 哈雷彗星 尾流 风差角 光度测量 日彗距 等离子体尾流
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返回舱再入段雷达散射特性研究 被引量:16
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作者 朱方 吕琼之 《现代雷达》 CSCD 北大核心 2008年第5期14-16,共3页
"神舟"飞船返回舱在再入过程中,由于产生等离子体鞘套和尾流,其雷达散射截面(RCS)出现剧烈变化,对地面测量雷达的跟踪产生影响。文中以C波段雷达的实测数据为依据,对返回舱RCS突增和缩减的机理进行了分析;重点阐述了厘米波雷... "神舟"飞船返回舱在再入过程中,由于产生等离子体鞘套和尾流,其雷达散射截面(RCS)出现剧烈变化,对地面测量雷达的跟踪产生影响。文中以C波段雷达的实测数据为依据,对返回舱RCS突增和缩减的机理进行了分析;重点阐述了厘米波雷达以反射式跟踪方式跟踪再入体时,会出现短时间目标丢失现象的必然性。 展开更多
关键词 再入返回舱 等离子体 等离子体尾流 雷达隐身 雷达散射截面
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THEMIS statistical study on the plasma properties of high-speed flows in Earth's magnetotail 被引量:2
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作者 PAN Dong Xiao SUN Wei Jie +6 位作者 SHI Quan Qi TIAN An Min YAO Zhong Hua FU Sui Yan ZONG Qiu Gang ZHOU Xu Zhi PU Zu Yin 《Science China Earth Sciences》 SCIE EI CAS CSCD 2016年第3期548-555,共8页
Using Time History of Events and Macroscale Interactions during Substorms (THEMIS) observations from 2007 to 2011 tail seasons, we study the plasma properties of high speed flows (HSFs) and background plasma sheet... Using Time History of Events and Macroscale Interactions during Substorms (THEMIS) observations from 2007 to 2011 tail seasons, we study the plasma properties of high speed flows (HSFs) and background plasma sheet events (BPSs) in Earth's magnetotail (|YGsM|〈13RE, |ZGsM|〈5RE, -30RE〈XrsM〈-6RE), and their correlations with solar wind parameters. Statistical results show that the closer the HSFs and BPSs are to the Earth, the hotter they become, and the temperature increase of HSFs is larger than that of BPSs. The density and temperature ratios between HSFs and BPSs are also larger when events are closer to Earth. We also find that the best correlations between the HSFs (BPSs) density and the solar wind density occur when the solar wind density is averaged 2 (3.5) hours prior to the onset of HSFs (BPSs). The normalized densities of both HSFs and BPSs are correlated with the interplanetary magnetic field (IMF) 0 angles ( 0 = arctan(Bz √Bx^2+y^2 ) which are averaged 3 hours before the observation time. Further analysis indicates that both HSFs and BPSs become denser during the northward IMF period. 展开更多
关键词 High-speed flow Earthward evolution Interplanetary magnetic field
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