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1.
利用资源一号卫星和神舟二号留轨舱上搭载的高能粒子探测设备对2001年2~6月同一时段内的资料进行了对比分析. 神舟二号飞船X射线探测器的观测结果反映的空间高能电子的分布, 表明在400km的较低高度上, 地理纬度40°附近以及SAA地区也可以观测到数百keV的高能电子. 资源一号卫星的探测结果显示了在800km高度附近, 同一时段内若干兆电子伏特的高能电子的全球分布. 后者出现的最低地理纬度和相应的经度位置则和前者是一致的, 说明两个高度上高能粒子的分布仍然都受地磁场控制, 粒子主要来源于地球辐射带. 资源一号卫星高能粒子探测器的能挡与神舟二号飞船X射线探测器的能挡不同, 彼此可以较好地补充. 但由于神舟二号轨道倾角较低, 全面的对比也受到一定的局限, 在进一步深入分析现有资料的同时, 可以在本文基础上设计更好的联合探测方案.  相似文献   

2.
2000年7月14日10:24UT一个X5.6级的耀斑暴发生在太阳中心子午线附近(AR 9077), 同时伴随着一个朝向地球的CME事件及太阳高能粒子(Solar Energetic Particle, SEP)事件. 这次耀斑暴发及CME事件引起了地球磁层、电离层及高层大气的强烈扰动. 中国“风云二号(B)”卫星上的高能粒子探测器(EPD)观测到SEP事件期间, 同步轨道区高能质子、相对论电子有非常剧烈的增加. SEP期间, 高能质子对相对论电子通量的探测造成严重的污染. 结合“风云二号(B)”卫星上的高能粒子探测器(EPD)的特性, 建立了一种从相对论电子通量探测中“清除”高能质子“污染”的方法, 并对相对论电子通量的探测数据实施“清洁”处理. “纯净的”相对论电子通量探测结果显示, 当行星际磁场南向时, 上游太阳风中的高能电子使同步轨道区相对论电子通量有大幅度的增加.  相似文献   

3.
风云二号系列卫星以自旋稳定方式工作于地球静止轨道,太阳X射线探测器是该系列卫星的重要有效载荷,监测太阳耀斑爆发过程,并对太阳质子事件等灾害性的空间天气事件进行预警.卫星自旋一周,该探测器完成一次全日面观测,记录太阳X射线的能谱与流量.2012年初,太阳活动进入第24周峰年,风云二号卫星太阳X射线探测器的在轨运行取得了良好的观测结果.相比于过去的太阳X射线探测器,风云二号F星的太阳X射线探测器应用了硅漂移探测(Silicon Drift Detector,SDD)技术,对GEO轨道海量的高能带电粒子采取了有效的屏蔽措施,可以对更"软"的X射线进行观测,能谱分辨率本领达到国际先进水平,对太阳耀斑的量化定级精度更高,在轨初步观测结果表明,精确的能谱探测能力可提高太阳质子事件预警能力,能道响应的时间特性比过去的探测数据更准确地反映了太阳耀斑的加热过程和带电粒子加速特性.本文介绍了风云二号F星太阳X射线探测器的设计及其发射前的标定试验结果,并且对发射后在轨运行获得的初步探测成果进行分析和讨论.  相似文献   

4.
本文比较了在太阳平静和扰动时期“资源一号”卫星星内粒子探测器对卫星舱内高能粒子的观测结果,发现在平静时期观测结果很好地反映了辐射带高能粒子在该高度上的分布情况.在扰动时期,粒子探测器观测到高能粒子分布出现重大变化,本文进一步讨论了影响高能粒子在近地空间分布的可能因素.  相似文献   

5.
星内粒子探测器观测结果与辐射带模型的比较   总被引:2,自引:0,他引:2       下载免费PDF全文
我们将资源一号卫星星内粒子探测器的观测数据与辐射带模式AE8/AP8的预测结果进行了对比,发现在南大西洋异常区的高能电子和质子的通量与辐射带模型的预测结果基本相同,而在两极极光带的电子通量比AE8模型预测的低得多.根据NOAA卫星的观测结果,可以认为这一差异主要是因为在南大西洋异常区(内辐射带)和两极极光带(外辐射带)的粒子投掷角分布的差异造成的.在南大西洋异常区粒子倾向于各向同性分布,而在极光带粒子各向异性明显,投掷角接近90°的粒子通量比0°投掷角附近的粒子通量大得多.  相似文献   

6.
FY 1C星空间粒子成分探测器能够实现对质子能谱、电子积分通量及重离子成分的同时测量.在第23周太阳活动峰年期间,空间粒子成分探测器对860km高度的南大西洋负磁异常区高能粒子辐射进行了长达3年的连续探测.本文根据实测结果,得出了南大西洋负磁异常区粒子辐射特征,分析了太阳质子事件和地磁暴对南大西洋负磁异常区粒子辐射的影响.  相似文献   

7.
FY2D卫星与GOES卫星空间粒子观测结果的对比分析   总被引:2,自引:1,他引:1       下载免费PDF全文
风云二号D星(FY2D)搭载的空间粒子探测器可以观测10~300 MeV的质子和≥350 keV与≥2 MeV的电子.卫星在轨测试阶段,空间粒子探测器观测到了空间环境宁静期间地球同步轨道的电子昼夜周期变化的典型特征,并在卫星发射后的12月15日首次观测到了有代表性的 2级太阳质子事件(SEP),观测到的较高能量质子比较低能量质子更快地恢复到平静时的状态.通过比较FY2D卫星与GOES卫星的探测结果,既显示了同步轨道区域不同位置高能电子通量扰动时间的一致性,也显示了高能电子通量具强烈的晨昏不对称性.通过对太阳质子事件和地磁平静时期该轨道空间高能粒子环境特征的分析和研究,并与GOES卫星同期的观测结果进行相关性分析,结果表明仪器确实具备了监测空间环境扰动和预警能力,探测结果可以用于研究地球同步轨道粒子空间分布、起源和传输等科学目的.  相似文献   

8.
“嫦娥一号”卫星太阳高能粒子探测器的首次观测结果   总被引:2,自引:0,他引:2  
"嫦娥一号"卫星(CE-1)的太阳高能粒子探测器(HPD)是国际上首次在200公里极月轨道观测高能带电粒子的探测仪器.HPD的科学目标是探测月球轨道空间的高能带电粒子(质子、电子和重离子)成分、能谱、通量和随时间的演化特征.通过比较分析HPD的观测结果、ACE卫星的观测结果与CRèME86模型的模拟计算结果,表明在太阳活动低年空间环境相对宁静时期,当月球处于太阳风中时,月球附近具有和行星际空间相近的宇宙线粒子流量背景.卫星在轨运行中发现了多起0.1~2MeV的高能电子流爆发事件.文中总结了2007年11月26日至2008年2月5日HPD观测的41起高能电子流爆发事件,发现此类现象可以发生在从太阳风到磁尾的所有空间区域.在月球经历的不同空间区域中,高能电子流爆发事件可能存在不同的诱发机制.  相似文献   

9.
JJI甚低频台站信号对太阳耀斑事件的响应特性   总被引:1,自引:0,他引:1  
太阳耀斑发生时,日地空间的X射线通量会随之增大,进而影响到地球电离层的电子密度分布,导致地球-电离层波导状态发生改变,因此接收到的甚低频(VLF,Very Low Frequency)信号会表现出对应的扰动现象.2017年9月8日,位于湖北省内武汉和随州两站点的VLF接收机分别监测到与X射线太阳耀斑相关的来自日本宫崎县(130°49′E,32°04′N)的JJI甚低频台站信号(22.2 kHz)的振幅异常事件.分析当日的数据发现JJI信号的振幅对不同的太阳耀斑出现不同的响应类型,而且对于同一个耀斑,两地的信号响应类型不尽相同.通过统计2017—2019年间与太阳耀斑相关的JJI信号振幅扰动事件,发现两接收站点的JJI信号响应类型都与耀斑强度及其发生时间存在一定的关系,且呈现出四种响应类型,即两次上升下降型、先上升后下降型、下降型和上升型,但是四种响应类型的事件占比不同.拟合结果表明信号的扰动幅度与X射线通量的积分成正相关,但是两站点的线性拟合斜率存在差异.JJI信号到武汉和随州均属于近似沿纬度方向的短距离传播,且两接收站点相距较近,因此两传播路径大致相似.研究两路径上JJI信号对太阳耀斑响应的差异性有助于理解VLF信号的传播以及探索其在太阳活动监测方面的应用.  相似文献   

10.
太阳质子事件期间内辐射带质子通量的变化   总被引:1,自引:0,他引:1  
本文介绍风云一号(B)卫星上的宇宙线成份监测器,在1991年1月30日及31目的耀斑期间及其前后几天,对能量在4-23MeV内的内辐射带质子通量的观测结果,并对这些结果做了详细的分析.结果表明,在这两次耀斑及其所产生的太阳质子事件期间,内辐射带质子通量有显著的变化:在磁漂移壳参量L≥1.64的空间,质子通量显著增强,增幅在40%-200%之间;在L=1.30-1.60的空间,质子通量的增强也较为明显,增幅在20%以上;总的变化趋势是,L越大的地方,质子通量的增强就越显著.质子事件之后,内辐射带质子通量又逐渐回复到质子事件之前平衡结构时的水平.  相似文献   

11.
A study was made of the polar cap absorption (PCA) event on 23–24 March 1991 produced by the largest solar proton event at E>10 MeV since August 1972. This PCA event was related to a solar flare in the eastern hemisphere lasting only 2 days and exhibiting a long time delay between the flare and the increase of ionospheric absorption. Midday recovery occurred regularly each PCA day near the cutoff lati- tudes during the noontime hours and is attributed to the daily variation in the proton cutoff latitudes. The maximum absorption during the PCA event was observed at high latitudes or near the cutoff latitudes where ionization may be due to both solar protons and trapped particles. The minimum in the absorption values during the night-time hours would appear to be caused by the chemistry of the D-region as well as access of the solar protons into the polar cap area.  相似文献   

12.
Ozone depression in the polar stratosphere during the energetic solar proton event on 4 August 1972 was observed by the backscattered ultraviolet (BUV) experiment on the Nimbus 4 satellite. Distinct asymmetries in the columnar ozone content, the amount of ozone depressions and their temporal variations above 4 mb level (38 km) were observed between the two hemispheres. The ozone destroying solar particles precipitate rather symmetrically into the two polar atmospheres due to the geomagnetic dipole field These asymmetries can be therefore ascribed to the differences mainly in dynamics and partly in the solar illumination and the vertical temperature structure between the summer and the winter polar atmospheres. The polar stratosphere is less disturbed and warmer in the summer hemisphere than the winter hemisphere since the propagation of planetary wave from the troposphere is inhibited by the wind system in the upper troposphere, and the air is heated by the prolonged solar insolation. Correspondingly, the temporal variations of stratospheric ozone depletion and its recovery appear to be smooth functions of time in the (northern) summer hemisphere and the undisturbed ozone amount is slighily, less than that of its counterpart. On the other hand, the tempotal variation of the upper stratospheric ozone in the winter polar atmosphere (southern hemisphere) indicates large amplitudes and irregularities due to the disturbances produced by upward propagating waves which prevail in the polar winter atmosphere. These characteristic differences between the two polar atmospheres are also evident in the vertical distributions of temperature and wind observed by balloons and rocker soundings.  相似文献   

13.
文中选了5 个典型活动区, 分析了这些活动区的磁场, 与活动区相应的CMEs, 太阳爆发事件和太阳质子事件我们发现, 对于E ≥10meV 的太阳质子事件有相应的源活动区, 源耀斑和CME; 活动区矢量磁场有剪切, 磁场剪切越强质子事件越强; 多数在质子耀斑发生前出现磁流浮现; 太阳10cm 射电爆发持续时间长文中结果还佐证了Shealy 等的结果: X 射线耀斑的长持续时间与CME 的发生正相关另外,在5 个活动区中, 有三个大耀斑发生前没有明显的磁剪切作为它们的先兆, 它们是非质子源耀斑这是Moore, Hagyard 和Davis 的磁场强剪切是耀斑产生的必要条件的反例  相似文献   

14.
Coronal mass ejections (CMEs) and solar flares are the large-scale and most energetic eruptive phenomena in our solar system and able to release a large quantity of plasma and magnetic flux from the solar atmosphere into the solar wind. When these high-speed magnetized plasmas along with the energetic particles arrive at the Earth, they may interact with the magnetosphere and ionosphere, and seriously affect the safety of human high-tech activities in outer space. The travel time of a CME to 1 AU is about 1–3 days, while energetic particles from the eruptions arrive even earlier. An efficient forecast of these phenomena therefore requires a clear detection of CMEs/flares at the stage as early as possible. To estimate the possibility of an eruption leading to a CME/flare, we need to elucidate some fundamental but elusive processes including in particular the origin and structures of CMEs/flares. Understanding these processes can not only improve the prediction of the occurrence of CMEs/flares and their effects on geospace and the heliosphere but also help understand the mass ejections and flares on other solar-type stars. The main purpose of this review is to address the origin and early structures of CMEs/flares, from multi-wavelength observational perspective. First of all, we start with the ongoing debate of whether the pre-eruptive configuration, i.e., a helical magnetic flux rope (MFR), of CMEs/flares exists before the eruption and then emphatically introduce observational manifestations of the MFR. Secondly, we elaborate on the possible formation mechanisms of the MFR through distinct ways. Thirdly, we discuss the initiation of the MFR and associated dynamics during its evolution toward the CME/flare. Finally, we come to some conclusions and put forward some prospects in the future.  相似文献   

15.
We performed a comparative study of geomagnetic variations, which are associated with sudden ionospheric disturbances (SIDs) caused by great X-class solar flares on July 14, 2000 (Bastille flare) and on October 28, 2003 (Halloween flare). Intense fluxes of solar X-rays and EUV radiation as well as solar energetic particles (SEP) were considered as sources of abundant ionization of the ionosphere and upper atmosphere. Flare-initiated SIDs are revealed as transient geomagnetic variations, which are generated by enhanced electric currents flowing mainly in the bottom-side ionosphere. Those so-called solar flare effects (SFEs) were studied by using of geomagnetic data from INTERMAGNET worldwide network of ground-based magnetometers. In subsolar region the SFE is mainly controlled by the flare X-rays and/or EUV radiation. We found that in the Halloween flare the contribution of X-rays was comparable with the EUV, but in the Bastille flare the EUV flux was dominant. The ionization at high latitudes is generated by the SEP, which energy flux is comparable and even exceeds the solar electromagnetic radiation in that region. It was shown that in the Halloween event the pattern of SFE is formed by a two-vortex current system, which is similar to the quiet day Sq current system. However, during the Bastille flare, the pattern of induced currents is quite different: the northern vortex shifts westward and southern vortex shifts eastward such that the electroject is substantially tilted relative to the geomagnetic equator. From numerical estimations we found that at middle latitudes the SEP-initiated geomagnetic effect becomes comparable with the effects of solar electromagnetic radiation. It was also shown that the SEP contribute to the SFE in the nightside hemisphere. The revealed features of the SEP impact to the ionosphere were found in a good agreement with the theory of energetic particle penetration to the bottom-side magnetosphere.  相似文献   

16.
The analysis of observations of large solar flares made it possible to propose a hypothesis on existence of a skin-layer in magnetic flux ropes of coronal mass ejections. On the assumption that the Bohm coefficient determines the diffusion of magnetic field, an estimate of the skin-layer thickness of ~106 cm is obtained. According to the hypothesis, the electric field of ~0.01–0.1 V/cm, having the nonzero component along the magnetic field of flux rope, arises for ~5 min in the surface layer of the eruptive flux rope during its ejection into the upper corona. The particle acceleration by the electric field to the energies of ~100 MeV/nucleon in the skin-layer of the flux rope leads to their precipitation along field lines to footpoints of the flux rope. The skin-layer presence induces helical or oval chromospheric emission at the ends of flare ribbons. The emission may be accompanied by hard X-ray radiation and by the production of gamma-ray line at the energy of 2.223 MeV (neutron capture line in the photosphere). The magnetic reconnection in the corona leads to a shift of the skin-layer of flux rope across the magnetic field. The area of precipitation of accelerated particles at the flux-rope footpoints expands in this case from the inside outward. This effect is traced in the chromosphere and in the transient region as the expanding helical emission structures. If the emission extends to the spot, a certain fraction of accelerated particles may be reflected from the magnetic barrier (in the magnetic field of the spot). In the case of exit into the interplanetary space, these particles may be recorded in the Earth’s orbit as solar proton events.  相似文献   

17.
本文统计了第22 太阳活动周期间(1991 ~1995 年) 发生的25 个太阳质子事件与太阳耀斑及日冕物质抛射(CME) 事件的关系  统计结果表明, 所有的太阳质子事件都与耀斑发生相关, 除2 个质子事件(19941020 和19951020 日发生的太阳质子事件) 与CME发生无关, 其余质子事件也都与CME 相关  值得注意的是, 与质子事件相关的耀斑有16 个是双带耀斑, 其中包括与CME无关的2 个事件的耀斑, 占总数的64 %   上述统计结果证实了无论是太阳耀斑, 还是物质抛射, 它们对太阳质子事件的发生同样起着非常重要的作用  相似文献   

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