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The substorm current wedge and midnight sector partial ring current near substorm onset: A synthesis based on a magnetotail magnetic field geometry model
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作者 George J Sofko Kathryn A McWilliams Chad R Bryant 《Advances in Polar Science》 2013年第1期32-41,共10页
The Substorm Current Wedge (SCW) occurrence in the late growth and onset phases of substorms was proposed as the current system which disrupts cross-tail current by diverting it to the ionosphere. The closure curren... The Substorm Current Wedge (SCW) occurrence in the late growth and onset phases of substorms was proposed as the current system which disrupts cross-tail current by diverting it to the ionosphere. The closure current for the SCW originally was suggested to be the strong westward auroral electrojet (WEJ). However, the SCW-WEJ system has no viable generator current. Similarly, the asymmetric or Partial Ring Current (PRC) increases in strength during the growth phase, and is sometimes associated with an enhanced Region 2 field-aligned current (FAC) closing to the ionosphere, but specifics of that closure have been lacking. Here we present a tmifying picture which includes the SCW post- and pre-midnight (AM and PM, respectively) currents and a generator current in the midnight portion of the PRC system, with these currents based upon a model of the nightside magnetotail magnetic geometry. That geometry consists of open north and south lobe regions surrounding a plasmasheet with two types of closed field line regions-stretched lines in the central part of the plasmasheet (SPS) and dipolar lines (DPS) between the low lati- tude boundary layer (LLBL) regions and the SPS. There is also an important plasmasheet transition region (TPS) in which the dipolar field near the plasmapause gradually transforms to stretched lines near the earthward edge of the SPS, and in which the midnight part of the PRC flows. We propose that our proposed near-onset current system consists of a central current which be- comes part of the midnight sector PRC and which is the generator, to which are linked two three-part current systems, one on the dawnside and one on the duskside. The three-part systems consist of up and down FACs closing as Pedersen currents in the iono- sphere. These 3-part systems are not activated until near-onset is reached, because of a lack of ionospheric conductivity in the appropriate locations where the Pedersen current closure occurs. The initial downward FAC of the 3-part dawnside system and the final upward FAC of the 3-part duskside system correspond to the AM and PM current segments, respectively, of the originally proposed SCW. 展开更多
关键词 MAGNETOTAIL magnetic field model auroral substorm substorm current wedge partial ring current substorm onset
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Observation evidence for the entropy switch model of substorm onset
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作者 YunXiang Song ChuXin Chen 《Earth and Planetary Physics》 EI CSCD 2022年第2期161-176,共16页
The cause of substorm onset is not yet understood. Chen CX(2016) proposed an entropy switch model, in which substorm onset results from the development of interchange instability. In this study, we sought observationa... The cause of substorm onset is not yet understood. Chen CX(2016) proposed an entropy switch model, in which substorm onset results from the development of interchange instability. In this study, we sought observational evidence for this model by using Time History of Events and Macroscale Interactions during Substorms(THEMIS) data. We examined two events, one with and the other without a streamer before substorm onset. In contrast to the stable magnetosphere, where the total magnetic field strength is a decreasing function and entropy is an increasing function of the downtail distance, in both events the total magnetic field strength and entropy were reversed before substorm onset. After onset, the total magnetic field strength, entropy, and other plasma quantities fluctuated. In addition, a statistical study was performed. By confining the events with THEMIS satellites located in the downtail region between ~8 and ~12 Earth radii, and 3 hours before and after midnight, we found the occurrence rate of the total magnetic field strength reversal to be 69% and the occurrence rate of entropy reversal to be 77% of the total 205 events. 展开更多
关键词 substorm onset entropy switch model interchange or ballooning instability Time History of Events and Macroscale Interactions during substorms(THEMIS)data
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The mid-high latitude whistler mode chorus waves observed around substorm onsets 被引量:6
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作者 YANG JunYing CAO JinBin +2 位作者 YAN ChunXiao LI LiuYuan MA YuDuan 《Science China(Technological Sciences)》 SCIE EI CAS 2008年第10期1648-1658,共11页
Using the data of LFEW/TC-2, we studied the dawn side chorus around substorm onsets during a strong geomagnetic storm in November 2004. During this storm, LFEW/TC-2 observed 14 dawnside chorus events. Nine of them wer... Using the data of LFEW/TC-2, we studied the dawn side chorus around substorm onsets during a strong geomagnetic storm in November 2004. During this storm, LFEW/TC-2 observed 14 dawnside chorus events. Nine of them were associated with substorms and occurred within 40 min around the substorm onsets. The fre-quencies of waves have a very good correlation with the half equatorial electron cyclotron frequencies. Chorus can be excited in the region near magnetic equato-rial plane and then propagate to the mid and high latitudes. When the wave fre-quencies reach the local lower hybrid frequencies, chorus can be reflected due to the lower hybrid resonance. The time delay between the chorus and its echo is about 28 min. Previous observations show that the chorus can propagate at most to the magnetic latitudes of 40°. LFEW/ TC-2 found for the first time that the chorus in space could propagate to the magnetic latitude of 70°. Since most of the previous chorus observations are made close to the magnetic equatorial plane, our results are important for the studies of excitation and propagation of whistler mode wave, and relevant relativistic electron acceleration in the magnetosphere. 展开更多
关键词 CHORUS substorm onset electron acceleration
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Observations of kinetic Alfvén waves by THEMIS near a substorm onset 被引量:5
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作者 DUAN SuPing LIU ZhenXing ANGELOPOULOS Vassilis 《Chinese Science Bulletin》 SCIE EI CAS 2012年第12期1429-1435,共7页
Low frequency electromagnetic fluctuations in the vicinity of a magnetospheric substorm onset were investigated using simultaneous observations by THEMIS multiple probes in the near-Earth plasma sheet in the magnetota... Low frequency electromagnetic fluctuations in the vicinity of a magnetospheric substorm onset were investigated using simultaneous observations by THEMIS multiple probes in the near-Earth plasma sheet in the magnetotail.The observations indicate that in the vicinity of a substorm onset,kinetic Alfvén waves can be excited in the high-βplasma sheet(β=2μ0nT/B 2 ,the ratio of plasma thermal pressure to magnetic pressure)within the near-Earth magnetotail.The kinetic Alfvén wave has a small spatial scale in the high-βplasma.The parallel electric field accompanying kinetic Alfvén waves accelerates the charged particles along the magnetic field.The kinetic Alfvén waves play an important role in the substorm trigger process,and possibly in the formation of a substorm current wedge. 展开更多
关键词 阿尔文波 动力学 暴发病 观测 等离子体片 亚暴电流楔 地球磁尾 空间尺度
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TC-1卫星在近地磁尾观测到的持续尾向流、等离子体片变薄和偶极化过程 被引量:2
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作者 王继业 张灵倩 +3 位作者 刘振兴 马志为 史建魁 郭九苓 《地球物理学进展》 CSCD 北大核心 2009年第4期1183-1188,共6页
2004年7月14日TC-1卫星在近地磁尾(-9.3Re,-5.4Re,1.2Re)附近观测到了伴随有持续尾向流s的等离体片变薄和偶极化过程.尾向流持续时间为32分钟.偶极化过程中磁场By分量没有明显变化.在偶极化过程发生两分钟之后,地面台站观测到的Pi2脉动.... 2004年7月14日TC-1卫星在近地磁尾(-9.3Re,-5.4Re,1.2Re)附近观测到了伴随有持续尾向流s的等离体片变薄和偶极化过程.尾向流持续时间为32分钟.偶极化过程中磁场By分量没有明显变化.在偶极化过程发生两分钟之后,地面台站观测到的Pi2脉动.ACE卫星的观测表明行星际磁场有弱的南向行星际磁场(-2nT),持续时间约55分钟.Imagine卫星在电离层区域没有观测到极光出现.和伴随有极光增亮的亚暴过程相比,南向行星际磁场明显较弱,且持续时间短.TC-1卫星和ACE卫星的联合观测表明尾部释能有大有小,并非达到某值才能发生.但能量小时,不能够引起极光亚暴.其次南向行星际磁场有可能与近地磁尾尾向流有密切关系. 展开更多
关键词 行星际磁场南转北 偶极化 亚暴膨胀相突发 Pi2脉动
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通量堆积和偶极化过程中的超低频波动 被引量:1
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作者 王继业 张灵倩 +3 位作者 刘振兴 马志为 史建魁 郭九苓 《地球物理学报》 SCIE EI CAS CSCD 北大核心 2008年第5期1285-1295,共11页
2004年9月17日TC-1卫星在近地磁尾夜侧观测到一次伴随有通量堆积和偶极化过程的典型亚暴事件.本文利用离散小波分析和FFT分析方法对本次事件中4s精度的FGM和HIA数据进行分析,以了解通量堆积过程和偶极化过程中的低频波特性.分析结果表明... 2004年9月17日TC-1卫星在近地磁尾夜侧观测到一次伴随有通量堆积和偶极化过程的典型亚暴事件.本文利用离散小波分析和FFT分析方法对本次事件中4s精度的FGM和HIA数据进行分析,以了解通量堆积过程和偶极化过程中的低频波特性.分析结果表明,通量堆积过程和偶极化过程中场和粒子有明显的不规则低频波动,主要波动频率范围为4~15mHz,和Pi-2脉动一致.通量堆积过程中磁场各个分量的低频波动和偶极化过程中的低频波动有明显不同,表明这两个物理过程可能存在不同的波动机制.在通量堆积过程和偶极化过程中,平行磁场方向上温度和速度的波动和垂直方向上温度和速度的波动有明显区别,平行磁场方向上温度和速度的波动有较好的相关性,且热离子密度的波动和平行磁场方向上的波动有较好的相关性,表明存在快模压缩波.TC-1卫星的观测显示通量堆积过程中磁场By分量有明显增长.我们的分析结果表明ULF波与By分量的增长有密切关系,从而可能对亚暴膨胀相的触发有重要影响. 展开更多
关键词 通量堆积 偶极化过程 膨胀相触发 超低频波(ULF)
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亚暴起始地磁指数判断的统计研究 被引量:1
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作者 丁维贞 曹晋滨 杜爱民 《空间科学学报》 CAS CSCD 北大核心 2010年第1期17-22,共6页
利用2004年地磁西向电急流AL指数,亚暴电急流AE指数和场向电流AF指数来确定亚暴起始,并与2004.年亚暴极光起始进行对比.研究发现,如果以极光亚暴起始为时间零点,亚暴的西向电急流AL起始和电急流AE起始主要分布于-5~+6min的时间范围内,... 利用2004年地磁西向电急流AL指数,亚暴电急流AE指数和场向电流AF指数来确定亚暴起始,并与2004.年亚暴极光起始进行对比.研究发现,如果以极光亚暴起始为时间零点,亚暴的西向电急流AL起始和电急流AE起始主要分布于-5~+6min的时间范围内,但在-9~+9min的时间范围内也有个别事例.场向电流AF起始分布较宽,可以分布于-8~+7min的时间范围内.平均西向电急流AL起始,电急流AE起始和场向电流AF起始分别为0.5,0.5,-0.1 min.通常西向电急流AL起始与极光起始同时的概率最高,而多数情况下电急流AE起始和场向电流AF起始提前极光起始1 min.这些地面磁场指数确定的亚暴起始分布,随着亚暴强度的增大(即最小AL指数减少,最大AE指数增大,最大AF指数增大)而向极光亚暴起始靠近.对于5个超级亚暴来说,其西向电急流AL起始和电急流AE起始都发生在极光起始之前.这些结果说明对于大亚暴,电急流的增加要早于极光爆发. 展开更多
关键词 亚暴 亚暴起始 AF指数 场向电流 AL指数
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中心等离子体片的地向对流型高速流
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作者 张灵倩 王继业 +1 位作者 刘振兴 史建魁 《空间科学学报》 CAS CSCD 北大核心 2011年第1期20-26,共7页
在GSM坐标系下,利用TC-1卫星和Cluster/C1卫星上4 s分辨率的磁场和热离子探测数据,对中心等离子体片内的地向对流型高速流进行了统计研究(-19R_e<x<-9R_e,|y|<10R_e,|z|<5R_e).统计结果表明,地向对流型高速流会在15R_e以内... 在GSM坐标系下,利用TC-1卫星和Cluster/C1卫星上4 s分辨率的磁场和热离子探测数据,对中心等离子体片内的地向对流型高速流进行了统计研究(-19R_e<x<-9R_e,|y|<10R_e,|z|<5R_e).统计结果表明,地向对流型高速流会在15R_e以内出现"刹车",在11.5R_e附近时出现"缺失".进一步对其速度特征进行统计分析.结果显示,在中心等离子体片内的高速流,其运动方向主要为地向,晨昏和南北方向的运动明显较弱;在对流型高速流的地向输运过程中,其峰值速度没有明显的下降;在近地13R_e以内,等离子体片内的地向对流型高速流具有较强的垂直磁力线运动速度.这意味着对流型高速流在近地15R_e以内的"刹车"不是由高速流晨昏或南北方向的偏转造成的.高速流在11.5R_e附近时出现的"缺失"可能与在15R_e以内出现"刹车"密切相关.TC-1卫星和Cluster卫星的观测为了解中磁尾重联高速流地向输运过程及亚暴膨胀相触发提供了重要的观测依据. 展开更多
关键词 近地磁尾 对流型高速流 中心等离子体片 亚暴膨胀相触发
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基于平均二次电子发射系数的航天器表面起电特征分析 被引量:3
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作者 方庆园 王通 +2 位作者 季启政 冯娜 刘卫东 《强激光与粒子束》 EI CAS CSCD 北大核心 2021年第2期77-82,共6页
为了进一步贴近航天器表面起电环境以得到更加可信的分析结果,针对航天器在恶劣充电环境下的表面起电问题,考虑空间等离子体双麦克斯韦分布情况,建立了基于平均二次电子发射系数的航天器表面起电阈值方程,可在入射电子能量连续分布情况... 为了进一步贴近航天器表面起电环境以得到更加可信的分析结果,针对航天器在恶劣充电环境下的表面起电问题,考虑空间等离子体双麦克斯韦分布情况,建立了基于平均二次电子发射系数的航天器表面起电阈值方程,可在入射电子能量连续分布情况下定量分析航天器表面起电特征,其中双麦分布可更好地描述磁层亚爆期间的恶劣充电环境。经过理论分析,归纳出双麦分布下的两种典型等离子体状态。通过仿真计算,得到了在两种典型等离子体状态下航天器表面电位随等离子体浓度和温度变化的特征。结果表明:电子温度越高,表面负带电电位越高,充电越严重,与此同时,双麦分布下等离子体两种电子组分的浓度比值对带电结果有重要影响。 展开更多
关键词 双麦分布 表面起电阈值 磁层亚爆 严重充电事件
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Correlation between continuous lobe reconnection in the mid magnetotail and substorm expansion onset
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作者 ZHANG Hui PU Zuyin +11 位作者 CAO Xin FU Suiyan XIAO Chijie LIU Zhenxing A. Korth M. Frazen ZONG Qiugong H. Reme K H Glassmeier R. Friedel G. D. Reeves M. W. Dunlop 《Chinese Science Bulletin》 SCIE EI CAS 2006年第22期2795-2804,共10页
Cluster/HIA 和 Cluster/FGM 在 2001 -2003 从 7 月在时期期间测量到 10 月的血浆表十字路口上的数据被分析。在连续脑叶的典型特征上基于以前的工作重新连接在参考,二案例研究和统计分析描述的离子(CLR ) 为发生在这个时期期间的事件... Cluster/HIA 和 Cluster/FGM 在 2001 -2003 从 7 月在时期期间测量到 10 月的血浆表十字路口上的数据被分析。在连续脑叶的典型特征上基于以前的工作重新连接在参考,二案例研究和统计分析描述的离子(CLR ) 为发生在这个时期期间的事件在 midmagnetotail 和潜水艇暴风雨扩大发作在在 CLR 之间的关联上被执行。几乎所有 CLR 事件在有潜水艇暴风雨的靠近的连接,这被发现。CLR 的开始几乎总是是在在近的地球磁电机尾巴并且在基于 theground 的车站上看见的潜水艇暴风雨活动前的一些分钟。这提供 CLR 在连续向南方的星际间的磁场的时期期间是 substormexpansion 发作的虚拟原因的一个清楚的指示。 展开更多
关键词 裂片重接 高速流 亚暴 特征性 统计分析 地磁学
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地球磁层亚暴统计分析
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作者 李世友 谢蓉 肖扬 《空间科学学报》 CAS CSCD 北大核心 2020年第6期1000-1006,共7页
利用AL和AE指数对第24个太阳活动周发生的亚暴事件进行统计分析.主要统计了关于磁层亚暴的强度,亚暴初值与恢复值的关系,亚暴持续时间,亚暴恢复相与增长相(包括膨胀相)持续时间的关系等.统计结果表明:在第24个太阳活动周中2008-2016年... 利用AL和AE指数对第24个太阳活动周发生的亚暴事件进行统计分析.主要统计了关于磁层亚暴的强度,亚暴初值与恢复值的关系,亚暴持续时间,亚暴恢复相与增长相(包括膨胀相)持续时间的关系等.统计结果表明:在第24个太阳活动周中2008-2016年发生的亚暴事件大部分比较剧烈,其峰值大都在200~1200nT;初值和恢复值大都在30~100nT,并且事件占比符合正态分布;大部分亚暴都能恢复到亚暴初值60nT以内,并且差值越小,事件的占比越大.大部分亚暴的持续时间较长,在100~400min之间,其中增长相(包括膨胀相)持续时间均在120min以内,并且持续时间越长,其事件占比越小;大部分亚暴事件的恢复相持续时间在60~300min之间,并且呈现出正态分布特征.绝大多数亚暴事件的恢复相持续时间为增长相持续时间的10倍以下,其中约一半亚暴事件的恢复相持续时间为增长相持续时间的1~4倍.这说明亚暴的能量聚集速度约为能量释放速度的1~4倍. 展开更多
关键词 亚暴强度 亚暴起始 亚暴持续时间 太阳活动周
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亚暴起始位置和膨胀相持续时间对行星际磁场Bz分量的响应
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作者 任干明 曹晋滨 马玉端 《空间科学学报》 CAS CSCD 北大核心 2022年第1期44-50,共7页
磁层亚暴是太阳风-磁层-电离层耦合过程中的重要爆发性事件,其特性受太阳风参数的影响很大。本文利用对IMAGE卫星在2000—2005年观测到的4193个亚暴起始事件,统计研究了在不同的行星际磁场(IMF)B;条件下亚暴起始位置和膨胀相持续时间。... 磁层亚暴是太阳风-磁层-电离层耦合过程中的重要爆发性事件,其特性受太阳风参数的影响很大。本文利用对IMAGE卫星在2000—2005年观测到的4193个亚暴起始事件,统计研究了在不同的行星际磁场(IMF)B;条件下亚暴起始位置和膨胀相持续时间。结果表明,南向IMF发生的亚暴比北向IMF下发生的亚暴要多。南向IMF条件下亚暴AE指数最大值的平均值基本上>600 nT,并有随南向IMF持续时间增大而增大的趋势。北向IMF条件下亚暴AE指数最大值的平均值基本上<500 nT,并有随北向IMF持续时间增大而减小的趋势。亚暴的起始磁纬度基本上位于65°—70°之间。当南向IMF或北向IMF的持续时间增大,超过80 min时,北半球的亚暴起始磁纬度会降低。亚暴起始磁地方时大部分位于22:15—23:15 MLT之间。但整体分布比较分散,显示不出特别清晰的随IMF B;持续时间变化的趋势。相比于南向的IMF,北向IMF期间发生亚暴的平均膨胀相持续时间增大了将近10 min,表明南向IMF期间,亚暴强度虽然较大,但其膨胀相持续时间较短,亚暴能量释放和耗散的速度更快。 展开更多
关键词 亚暴起始 磁地方时 磁纬度 膨胀相持续时间
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Continuous tailward flow in the near-Earth magnetotail observed by TC-1 satellite 被引量:3
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作者 HANG LingQian LIU ZhenXing +3 位作者 MA ZhiWei PU ZuYin WANG JiYe SHEN Chao 《Chinese Science Bulletin》 SCIE EI CAS 2007年第14期1980-1985,共6页
On July 11, 2004, a substorm process in the period of continuous tailward flow was observed by the joint exploration of the TC-1, IMAGE and ACE satellites. The substorm observed by the TC-1 in the near-Earth has three... On July 11, 2004, a substorm process in the period of continuous tailward flow was observed by the joint exploration of the TC-1, IMAGE and ACE satellites. The substorm observed by the TC-1 in the near-Earth has three stages: the growth phase (from 11:43 to 12:19), the pre-expansion process (from 12:19 to 12:28) and the dipolarization process. The auroral brightening was at 12:26 recorded by the FUV instrument on IMAGE, and the dipolarization occurred two minutes later. During the 45 min period of the tailward flow, the magnetotail experienced the growth phase and the pre-expansion process. When the dipolarization process began, the TC-1 entered the plasma sheet and observed a high speed earthward flow. The field-aligned tailward flow is characterized by the low temperature and high density, which is consistent with the properties of the flow from the ionosphere detected in the near-Earth magnetotail by other satellites. The tailward flow is closely related with the southward interplanetary magnetic field (IMF), and may have an important effect on the substorm. 展开更多
关键词 风暴 磁层尾 人造卫星 气候
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Near-Earth bursty bulk flows and AE index 被引量:1
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作者 W BAUMJOHANN M. W. DUNLOP +1 位作者 C. CARR H. RME 《Science China(Technological Sciences)》 SCIE EI CAS 2008年第10期1704-1712,共9页
With the 4-s resolution data of the magnetometer and the ion plasma analyzer on TC-1 from June to November of each year during the period of 2004―2006, we statistically analyzed the occurrence rate of both convective... With the 4-s resolution data of the magnetometer and the ion plasma analyzer on TC-1 from June to November of each year during the period of 2004―2006, we statistically analyzed the occurrence rate of both convective and field-aligned bursty flows (FABFs). A near-Earth bursty bulk flow (NEBBF) occurred during both the quiet time and substorm process. In general, the magnetic field and the plasma density began oscillating with the appearance of the NEBBF associated with a distinct increase of the AE index. The increase of AE index during the NEBBF was more than 100 nT in both quiet time and substorm process. The statistical analysis indicated that the occurrence rates of the FABFs were nearly the same in the dif-ferent stages of the AE index, but the occurrence rate of the NEBBFs was much higher in the growth stage of the AE index, indicating that the NEBBFs were di-rectly related to the growth and expansion phases of the substorm. The observa-tions suggested that the quite large number of BBFs from the mid magnetotail could enter into the near-Earth tail and play important role in triggering the sub-storm onset. 展开更多
关键词 BBF near-Earth AE INDEX substorm onset
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