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国家自然科学基金(40831060)

作品数:6 被引量:11H指数:2
相关作者:王赤李晖张北辰王继业更多>>
相关机构:中国科学院中国极地研究中心中国科学院研究生院更多>>
发文基金:国家自然科学基金国家重点基础研究发展计划国家重点实验室开放基金更多>>
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6 条 记 录,以下是 1-6
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Effect of the Interplanetary Electric Field on the Magnetopause From Global MHD Simulations
2012年
The north-south component B_z of the Interplanetary Magnetic Field(IMF) and solar wind dynamic pressure P_d are generally treated as the two main factors in the solar wind that determine the geometry of the magnetosphere.By using the 3D global MHD simulations,we investigate the effect of the Interplanetary Electric Field(IEF) on the size and shape of magnetopause quantitatively. Our numerical experiments confirm that the geometry of the magnetopause are mainly determined by P_d and B_z,as expected.However,the dawn-dusk IEFs have great impact on the magnetopause erosion because of the magnetic reconnection,thus affecting the size and shape of the magnetopause.Higher solar wind speed with the same B_z will lead to bigger dawn-dusk IEFs,which means the higher reconnection rate,and then results in more magnetic flux removal from the dayside. Consequently,the dayside magnetopause moves inward and flank magnetopause moves outward.
HUANG ZhaohuiDING KaiWANG Chi
关键词:磁层顶MHD行星际磁场太阳风
太阳风一磁层相互作用的磁流体力学数值模拟研究被引量:8
2011年
磁层位于地球空间的最外层,太阳风与磁层的相互作用是空间天气变化因果链中承上启下的关键环节,是揭示地球空间天气基本规律的关键科学课题.地球空间由于时变、多成分、多自由度的关联相互作用,使得传统的理论分析变得非常困难.数值模拟作为近几十年发展起来的一个新的研究手段,对地球空间的理论和应用研究产生了深刻的影响.国际上磁层的全球MHD数值模拟工作开始于20世纪70年代末,最初的研究局限于二维空间由于磁层内在的三维特性,20世纪80年代三维MHD数值模拟工作兴起.本文简要说明了三维全球磁层MHD(磁流体力学)研究的特点及现状,给出了三维全球磁层模型的基本框架,综述了行星际激波与磁层相互作用、大尺度电流体系、重联电压和越极电位、磁层顶K-H不稳定性等方面的太阳风-磁层相互作用的MHD数值模拟的研究进展.
王赤
关键词:磁流体力学数值模拟
Numerical study on the response of the Earth's magnetosphere-ionosphere system to a super solar storm被引量:3
2012年
With the approaching of the 24th solar cycle peak year (2012-2014), the impacts of super solar storms on the geospace environment have drawn attentions. Based on the geomagnetic field observations during Carrington event in 1859, we estimate the interplanetary solar wind conditions at that time, and investigate the response of the magnetosphere-ionosphere system to this extreme solar wind conditions using global 3D MHD simulations. The main findings include: 1) The day-side magnetopause and bow shock are compressed to 4.3 and 6.0 Re (Earth radius), and their flanks are also strongly compressed. The magnetopause shifts inside the geosynchronous orbit, exposing geosynchronous satellites in the solar wind in the magnetosheath. 2) During the storm, the region-1 current increases by about 60 times, and the cross polar potential drop increases by about 80 times; the reconnection voltage is about 5 to 6 times larger than the average storms, which means a larger amount of the solar wind energy enters the magnetosphere, resulting in strong space weather phenomena.
WANGChiLI HuiGUO XiaoChengDING KaiHUANG ZhaoHui
关键词:太阳风暴地球磁层地球同步轨道太阳活动周期
Electrodynamic Coupling in the Solar Wind-Magnetosphere-Ionosphere System被引量:2
2010年
This paper presents a brief summary of our recent work based on global MHD simulations of the Solar wind-Magnetosphere-Ionosphere (SMI) system with emphasis on the electrodynamic coupling in the system.The main conclusions obtained are summarized as follows.(1) As a main dynamo of the SMI system,the bow shock contributes to both region 1 Field-Aligned Current (FAC) and cross-tail current.Under strong interplanetary driving conditions and moderate Alfv'en Mach numbers,the bow shock's contribution may exceed more than fifty percent of the total of either region 1 or cross-tail currents.(2) In terms of more than 100 simulation runs with due southward Interplanetary Magnetic Field (IMF),we have found a combined parameter f=E sw P sw M A -1/2 (E sw,P sw,and M A are the solar wind electric field,ram pressure,and Alfv'en Mach number,respectively):both the ionospheric transpolar potential and the magnetopause reconnection voltage vary linearly with f for small f,but saturate for large f.(3) The reconnection voltage is approximately fitted by sin 3/2 (θ IMF /2),where θ IMF is the IMF clock angle.The ionospheric transpolar potential,the voltage along the polar cap boundary,and the electric fields along the merging line however defined they may be,respond differently to θ IMF,so it is not justified to take them as substitutes for the reconnection voltage.
Hu YouqiuWang Chi
关键词:太阳风磁层顶行星际磁场场向电流
中心等离子体片的地向对流型高速流
2011年
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
张灵倩王继业刘振兴史建魁
关键词:近地磁尾
基于T96模型的极尖区位形变化特性研究被引量:1
2012年
基于T96模型,定义了极尖区的位形以及相关的描述参量(例如赤道向边界磁纬的最小值,纬向宽度,子午向和晨昏向的张角,倾斜度,扁平度,中心磁地方时等),讨论了太阳风动压(P_d)、行星际磁场(IMF)及磁暴强度对极尖区位形的影响.太阳风动压和磁暴强度越大,则极尖区的赤道向边界磁纬越小,纬向宽度越大,子午向和晨昏向的张角越大,倾斜度越大,扁平度越小;南向IMF B_z越强,则极尖区的赤道向边界磁纬越小,纬向宽度越小,子午向的张角越小,晨昏向的张角越大,倾斜度越大,扁平度越大;北向IMF B_z与南向IMF B_z的情况刚好相反;极尖区的中心磁地方时受IMF B_y控制,IMF B_y为正时,极尖区向昏侧移动,而IMF B_y为负时,极尖区则向晨侧移动,并且极尖区的中心磁地方时与IMF B_y之间有着良好的线性关系.将所得结果与前人的观测结果进行了简单比较,发现利用T96模型确定的极尖区位形与观测基本一致.
李晖王赤张北辰
关键词:极尖区行星际扰动
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