Study of the longitudinal expansion velocity of the substorm current wedge     

A. Belehaki  I. Tsagouri  H. Mavromichalaki 《Annales Geophysicae》1998,16(11):1423-1433

In this work we examine simultaneous observations from the two geosynchronous satellites GOES-5 and GOES-6 located at 282°E and 265°E respectively, and from middle and low latitude ground observatories located within 250°E and 294°E geographic longitude, during isolated substorms of moderate activity. The spatial distribution of our observation points allows us to make a detailed study of the azimuthal expansion of the substorm current wedge. The data analysis shows evidence that the substorm initiation and development mechanism include the cross-tail current diversion/disruption, the substorm current wedge formation and the azimuthal expansion of the inner plasma sheet. The triggering mechanism is initially confined in a longitudinally narrow sector, estimated to be less than 15° and located very close to local midnight to the east or to the west. The current disruption region expands both eastward and westward in the magnetotail, so that the location of major field-aligned currents flowing into the ionosphere shifts successively eastward, and the location of the currents flowing out of the ionosphere shifts successively westward. Evidence was found that the perturbation travels toward the west with velocities greater than those expanding the wedge eastward. The drastic decrease of the velocity with the azimuthal distance from the location of the disturbance initiation, i.e., the onset sector, indicates that the energy release is a very localized phenomenon. Finally, the transient D perturbation observed by the geosynchronous satellites suggests that the field-aligned currents forming the wedge have a longitudunally limited extent.  相似文献   

The distribution characteristics of short period geomagnetic variations in Shaanxi region     

GUO HUA FAN TONG QI YAO KE LI HAN KE JIA ZHU ZUO WEN GU Institute of Geophysics  China Seismological Bureau  Beijing  China 《地震学报(英文版)》1998,11(6):719-727

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电阻率层析成像方法技术近年发展概况   总被引：15，自引：7，他引：8  

杨华  李金铭 《地球物理学进展》1998,13(4):90-96

本文对近年来电阻率层析成像在方法技术方面的进展作了简要介绍,并对几种具有代表性的方法,表述了它们各自的优缺点,提出了继续研究的方向。  相似文献   

Bottom-current deposits in the Miocene–Pliocene Misaki Formation, Izu forearc area, Japan     

INTAE  LEE & YUJIRO  OGAWA 《Island Arc》1998,7(3):315-329

Sedimentary structures in the middle–late Miocene to early Pliocene Misaki Formation, Miura Group, Miura Peninsula, Central Japan, were studied, and paleocurrent data were interpreted as the result of deep-sea bottom-current flow. These current data were further compared with present-day bottom currents in the northwestern Pacific region. The Misaki Formation is thought to be a forearc deposit within the Izu oceanic arc, and is composed of thick volcaniclastic beds interbedded with siliceous biogenic clayey sediments. Sedimentary structures showing paleocurrent directions are involved in the upper part of the volcaniclastic beds, in the pumiceous beds just above the volcaniclastic beds, and in the pelagic sediments. Based on paleomagnetic data suggesting considerable rotation of the beds, all the current directions were reconstructed to their original orientation. The paleocurrents are summarized into the following three groups. The first group in the volcaniclastic beds indicates southeast-directed paleocurrent directions. The second group in the upper parts of volcaniclastic beds and in some pumiceous beds exhibits a southwest- and northeast-directed paleoflow. The third group usually observed in the pumiceous beds with parallel lamination displays a northwest- or southeast-directed paleocurrent. The origin of each group's paleoflow direction is attributed to turbidity current, internal tidal current, and contour current influences, respectively. Present-day observations of the deep-sea northwest Pacific suggest that most of the bottom-current indicators in the Misaki Formation are related to North Pacific Deep Water, possibly Antarctic Bottom Water as well as a combination of tidal and local effects. It is concluded that the beds of the Misaki Formation were deposited in the proto-Sagami basin ca 9 Ma and were formed under weak bottom currents in a wide and flat basin during colder climatic conditions, whereas the beds dated at ca 6 Ma were deposited under strong bottom-current flow, and were then accreted to the Honshu arc.  相似文献   

浊流及相关重力流沉积研究综述   总被引：44，自引：2，他引：42  

方爱民  李继亮 《地质论评》1998,44(3):270-280

本文首先介绍了浊流及相关重力流的有关概念,并对浊流沉积研究历史进行了简要回顾,概括了当前浊流沉积的研究现状;随后,总结了浊积岩的沉积特征并对其成因进行了扼要解释;最后,对浊流及相关重力流沉积研究中两个有争议的问题－浊积相的划分和浊积相模式的建立进行了探讨。  相似文献   

对计算土壤和岩石中氡浓度及其表面析出率表面边界条件的讨论     

何斌  过惠平 《铀矿地质》1998,14(5):302-307

本文对求解土壤或岩石中氡浓度及其表面析出率的边界条件进行了探讨。以空气中无穷远处氡浓度为零（空气中无氡源）的自然边界条件代替空气与土壤或岩石交界面氡浓度为零的边界条件,给出了土壤和岩石中氡浓度及其表面析出率的具体表达式。与前人研究结果比较,该式中增加了一项,表面氡析出率缩小了一个倍数。通过对土壤、岩石的具体计算．表明两种边界条件的计算结果有相当的偏差。同时,文中还讨论了在两类边界条件下对流对土壤或岩石中氡浓度及其表面析出率计算的影响。  相似文献   

极光区高空物理过程与磁层-电离层耦合   总被引：1，自引：1，他引：0       下载免费PDF全文

沈长寿  资民筠 《极地研究》1998,10(4):57-67

极区高空物理现象之观测具有悠久历史。对极区地磁、电离层和极光现象的深入考察将地球物理的研究领域扩展到了外层空间,并提出了太阳风－磁层－电离层－热层间耦合这一重要课题。耦合物理机制的证实不仅是火箭、卫星探测的重要贡献,而且也是基于对地面雷达和遍及全球大陆的地磁台站、电离层垂测站之长期观测成果。对流电场、一区和二区场向电流、电离层扰动电流系（包括极光区电集流）,以及电导率的分布和变化乃是一有机整体,对其每一环节的深入认识均与对整体的全面了解密不可分。有关的理论和模式研究则有助于人们深入理解各个耦合过程的相互关系,以及其各发展阶段中不同物理过程的相对重要性。  相似文献   

电偶源电场的时间谱转换为频谱的误差探讨     

昌彦君  罗延钟 《物探化探计算技术》1998,(2)

基于层状导电和可极化大地表面,电偶源电场的时间谱在无随机干扰和有随机干扰时,进行频谱转换的计算结果,证明了时—频转换的误差传递问题严重。但是,采用窗口（圆滑）滤波可以有效压制随机干扰,使时—频转换达到必要的计算精度。  相似文献   

基于LLS的多回击地闪及其雷电流幅值分布特征     

王学良  成勤  王清龙  余田野  张科杰  赵涛 《热带气象学报》2021,37(3):309-319

为进一步研究多回击地闪参数分布特征, 以便为雷电防护工程设计和雷电物理研究提供参考, 根据湖北省雷电定位系统(LLS)2007年1月—2018年12月监测资料, 采用计算机编程处理和数理统计方法, 对多回击地闪次数、多重回击次数和不同类型多回击地闪雷电流幅值等参数进行了统计分析。结果表明: 多回击正地闪、负地闪和总地闪次数占其地闪总数的百分比分别为2.06%、34.76%和32.64%, 多重回击次数分别占其回击总数的0.01%、0.42%和0.40%, 多回击负地闪回击次数占多回击总地闪回击总数的99.69%。首次回击强度大于后续回击强度的多回击正地闪和负地闪分别占多回击地闪总数的82.52%和57.87%;在多回击地闪后续回击中, 正地闪约有9%的后续回击强度大于首次回击强度, 负地闪约有20%的后续回击强度大于首次回击强度。多回击正地闪和负地闪中值电流分别为59.30 kA和35.10 kA, 首次回击分别为90.90 kA和40.00 kA, 后续回击中分别为43.90 kA和33.00 kA。首次回击中, 多回击正地闪和负地闪雷电流幅值大于100 kA的累积概率分别为44.06%和4.64%, 首次回击强度大于后续回击强度的多回击正地闪和负地闪雷电流幅值大于100 kA的累积概率最大分别为52.21%和7.94%;后续回击中, 多回击正地闪和负地闪雷电流幅值小于等于40 kA的累积概率分别为41.80%和69.92%, 首次回击强度大于后续回击强度的多回击负地闪, 雷电流幅值小于等于40 kA的累积概率最大为77.71%。多回击正地闪和负地闪后续回击与首次回击中值电流的比值分别为0.48和0.83。拟合得出的不同类型的多回击正地闪和负地闪雷电流幅值累积概率公式, 拟合效果显著; 拟合公式中a值附近的雷电流幅值累积概率与b值呈显著正相关关系。   相似文献   

基于K-Means算法的架空输电线路载流量计算     

林锦荣  武云发  廖如超  陈郑淦哲 《南京气象学院学报》2021,13(1):73-78

针对边界条件取值过于保守导致架空输电线路载流量过小而无法充分发挥输电线路的载流能力的问题,本文提出了一种基于K-Means算法的架空输电线路载流量计算方法.首先对历史气象数据进行统计分析,然后根据每月气象数据的相似性,使用K-Means算法划分时段,并选取各时段最为合适的边界条件,最后基于选定的边界条件使用摩根公式进行仿真计算.通过这种方法,可以在保证线路运行安全的条件下挖掘输电线路的隐性输送能力.  相似文献