Ray Structure of the Coronal Streamer Belt and Its Manifestation as Sharp Large Peaks of Solar Wind

来源 :空间科学学报 | 被引量 : 0次 | 上传用户:jh_viso1
下载到本地 , 更方便阅读
声明 : 本文档内容版权归属内容提供方 , 如果您对本文有版权争议 , 可与客服联系进行内容授权或下架
论文部分内容阅读
The white-light corona calibrated data with processing level L1 from the LASCO-C2/SOHO instrument, and data from the Wind spacecraft with one-hour and one-minute time resolution on quasi-stationary slow (v between 300-450 km/s at the Earth's orbit) the Solar Wind (SW) parameters in the absence of sporadic SW streams are examined. Within distances from the Sun's center less than R in the range of 20-30 Rs,(Rs, the solar radius), slow wind is known as the streamer belt, and at larger distances it is called the Heliospheric Plasma Sheet (HPS). It is shown that the streamer belt comprises a sequence of pairs of rays. In general, ray brightnesses in each pair can differ, and the magnetic field is oppositely directed in them. The neutral line of the radial magnetic field of the Sun runs along the belt between the rays of each of the pairs.The area in which the streamer belt intersects the ecliptic plane and which lies at the central meridian, will be recorded at the earth's orbit with a time delay of 5-6 days, in the form of one or several peaks with Nmax > 10 cm-3. Furthermore, the simplest density profile of the portion of the HCS has the form of two peaks of a different or identical amplitude . The such a profile is observed in cases where the angle of intersection of the streamer belt with the ecliptic plane near the Sun is sufficiently large, i.e. close to 90°. The two-ray structure of the cross-section of the streamer-belt moves from the Sun to the Earth, it retains not only the angular size of the peaks but also the relative density variations, and the position of the neutral line(sector boundary) in between. At the Earth's orbit the ray structure of the streamer belt provides the source for sharp (i.e. with steep fronts of a duration of a few minutes or shorter) solar wind plasma density peaks (of a duration of several hours) with maximum values Nmax > 10 cm-3.
其他文献
利用M-LDARS闪电定位系统对北京及其周边地区1995~1997年6~9月的闪电观测数据,分析闪电活动的时空分布特征.结果表明:闪电活动在时间分布上存在两个峰值时段,13:00~21:00和23:00
以南华北盆地户部寨第三系沙河阶组粉砂岩低渗透储层为例,总结了其中发育的5种类型构造裂缝组合,即:①南北向雁形张节理组成的共轭剪节理带;②东西向雁形张节理组成的共轭剪
以大陆动力学、构造地质学和含油气系统理论做指导,以盆地构造-沉积分析技术为手段,研究了塔东地区与南天山、阿尔金山之间的耦合关系,探讨了塔东地区的大地构造演化特征及其
对采用美国国家沥青技术中心(NCAT)燃烧炉法测定沥青混合料中沥青含量的几种影响因素进行分析,并论述燃烧炉法测定沥青含量在实际生产中的优点,从而使测量结果更趋于合理和准
用SSA方法分析了哈尔滨1909-2002年94 a月平均气温距平序列,其气温总的倾向是增温的,升温约1.54 ℃,主要的年代尺度增温时段是1918-1952年升温约0.53 ℃,1971-2002年升温约1.
An analysis of the data from the Wind and IMP-8 spacecraft revealed that a slow solar wind, flowing in the heliospheric plasma sheet, represents a set of magnet
首先论述了近年来飞速发展的Web GIS的现状及面临的技术难点,然后介绍XML(Extensible Markup Language),GML(Geography Marker Language),SVG(Scalable Vector Graphics)的发
This paper presents convincing evidence for the reality of manifestations of solar variability in climate characteristics of the Prebaikalia. A numerical estima
The five main types of antisunward propagating energetic fluxes (particles and emission) may be thought of as well established to date, the effects of which lea
求取裂缝性油藏裂缝孔隙度的方法通常是先通过成像测井识别和拾取出高导缝,然后再利用成像测井对常规测井识别的裂缝和计算的裂缝孔隙度进行标定.在缺少成像测井资料的情况下