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1.
亚暴期间高纬黄昏-子夜扇区极光弧增亮与衰减及其与IMF的关系 总被引：3，自引：0，他引：3
利用南极中山站极光全天空摄相、地磁、地磁脉动数据和Wind卫星的行星际磁场IMF观测数据，分析了7个亚暴期间高纬黄昏-子夜扇区极光弧的短暂增亮现象.极光弧特征是，短暂增亮随后很快衰减，历时10-20min，基本沿着日-地方向，有明显黄昏方向运动.这些事件大都发生在IMFBz南转之后，亚暴增长相或膨胀相期间，极光浪涌到达之前10-73min消失.相应的IMFBx＞0，IMFBy＜0.这种极光弧和亚暴极光不同，它们与地磁活动及Pi2脉动不相关.这7个极光弧的形态和IMF特征表明，极光弧的增亮很可能由尾瓣重联产生，很快衰减归因于IMFBz南向条件，而黄昏方向运动受IMFBy控制. 相似文献
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《中国科学:地球科学》2017,(2)
极光是磁层与电离层-热层复杂相互作用的直观表现,对极光进行合理分类有助于了解极光发生机制及其与磁层边界层动力学过程之间的相互关系.面对逐年增长的海量极光数据,亟需自动的极光分类方法.本文基于韦伯局部描述符(WLD)提出了一种极光图像描述方法,该方法能表征全天空极光图像的纹理、形状和亮度等形态特征.基于该方法,对2003~2009年北极黄河站越冬观测的4种日侧极光类型进行自动分类.在2003年8001幅典型极光图像上,与人工标记对比分类准确率高达94.8%,高于其他同类方法;对2004~2009年越冬观测数据进行自动识别,获得4种极光类型的发生分布与日侧极光的多波段能量分布一致.实验结果表明本文方法能有效用于极光图像表征,为海量极光图像自动分类提供了一种新方法. 相似文献
3.
为研究极光电集流地磁纬度分布特征,利用北半球SME台站提供的极光电集流指数,通过时序叠加的方法,分析98-07年极光电集流中心地磁纬度随季节和世界时的分布特征.通过对磁扰程度的分级,分析极光电集流地磁纬度随地磁扰动程度的变化特征.结果表明:1)由于SME台站覆盖范围更广,更多地记录到最大的极光电集流强度,有利于研究极光电集流的变化特征;2)西向板光电集流纬度分布存在与强度相反的季节性变化特征,在春秋出现最低值,冬季、夏季出现最高值;3)在| SML|＜2000 nT时,西向极光电集流地磁纬度随着极光电集流强度的增强,近似以线性关系向低纬迁移.随后伴随SML的进一步增强,西向极光极光电集流中心地磁纬度仍有向低纬迁移的趋势,但主要是在磁纬62°N-63°N之间波动. 相似文献
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5.
对川滇及邻区特定构造区域地震活动的时间、强度和空间分布进行了分析,结合研究区1988年以来的8次地震发生前ML≥3.0级地震活动指标缺震(L值)、频度(N值)、活动度(S值)和危险度(D值)的曲线非线性特征进行了分析,给出了下一次地震危险性时间的估计方法。川滇及相邻地区的地震模型ML≥3.0级群体地震活动的震兆曲线,能够很好地描述川滇区域地震活动强、弱变化的异常信息,临震信号是地震失稳的标志,有震异常和临震前的短临异常反映出的时间变化非线性曲线特征能够有效地给出地震发生的时间判断。 相似文献
6.
《地球物理学进展》2017,(5)
地磁规则日变化的有效提取能够提高地磁活动指数现报的准确性.本文基于1998—2013年北京十三陵(BMT)台站的地磁数据,利用卡尔曼滤波(KF)方法提取了地磁场规则日变化(S_R)曲线.该方法提取的S_R曲线具有明显的逐日变化特征,能够准确反映S_R曲线的季节变化和地方时效应.根据KF方法得到的S_R日变幅度逐日变化的结果,改进了K指数的量算方法,重新计算了十三陵台站的K指数以及Ak指数,并分析了S_R日变幅度的逐日变化对K指数量算的改进程度.分析结果表明,当K≤3时,KF方法可以较好地改善S_R曲线扰动幅度的计算,提高了地磁规则日变化提取的有效性,从而改进相应的地磁活动指数的量算. 相似文献
7.
根据网络工程的GPS站点观测资料,计算相对中国大陆整体1999～2007年的趋势运动速率和2004~2007年的动态运动速率,用青藏亚板块和华南亚板块的参数计算龙门山断裂带的活动参量,研究了中国大陆运动场和其变化,分析了地壳运动场的特征与汶川MS8级地震的孕育关系.结果揭示出：现今地壳的运动分区与地质新构造单元基本一致,显示现代地壳构造活动是新构造运动的继承和发展;中国大陆地壳运动的动力主要与印度板块、太平洋板块与欧亚板块的相互碰撞俯冲产生的作用力有关.汶川MS8级地震的发生,主要是由于印度板块对青藏亚板块的向北推挤、产生侧向运动,致使龙门山断裂带遭受挤压产生能量积累所致.2004～2007年的地壳动态运动,使龙门山断裂带走滑活动加强,从稳定的压应变积累状态转入了剪切作用下的易活动状态. 相似文献
8.
根据网络工程的GPS站点观测资料,计算相对中国大陆整体1999～2007年的趋势运动速率和2004～2007年的动态运动速率,用青藏亚板块和华南亚板块的参数计算龙门山断裂带的活动参量,研究了中国大陆运动场和其变化,分析了地壳运动场的特征与汶川Ms8级地震的孕育关系.结果揭示出:现今地壳的运动分区与地质新构造单元基本一致,显示现代地壳构造活动足新构造运动的继承和发展;中国大陆地壳运动的动力主要与印度板块、太平洋板块与欧亚板块的相互碰撞俯冲产生的作用力有关.汶川Ms8级地震的发生,主要是由于印度板块对青藏亚板块的向北推挤、产生侧向运动,致使龙门山断裂带遭受挤压产生能量积累所致.2004～2007年的地壳动态运动,使龙门山断裂带走滑活动加强,从稳定的压应变积累状态转入了剪切作用下的易活动状态. 相似文献
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L. A. Hajkowicz 《Annales Geophysicae》1998,16(12):1573-1579
Statistical study on the universal time variations in the mean hourly auroral electrojet index (AE-index) has been undertaken for a 21 y period over two solar cycles (1957–1968 and 1978–1986). The analysis, applied to isolated auroral substorm onsets (inferred from rapid variations in the AE-index) and to the bulk of the AE data, indicates that the maximum in auroral activity is largely confined to 09–18 UT, with a distinct minimum at 03–06 UT. The diurnal effect was clearly present throughout all seasons in the first cycle but was mainly limited to northern winter in the second cycle. Severe storms (AE > 1000 nT) tended to occur between 9–18 UT irrespective of the seasons whereas all larger magnetic disturbances (AE > 500 nT) tended to occur in this time interval mostly in winter. On the whole the diurnal trend was strong in winter, intermediate at equinox and weak in summer. The implication of this study is that Eastern Siberia, Japan and Australia are mostly at night, during the period of maximum auroral activity whereas Europe and Eastern America are then mostly at daytime. The minimum of auroral activity coincides with near-midnight conditions in Eastern America. It appears that the diurnal UT distribution in the AE-index reflects a diurnal change between interplanetary magnetic field orientation and the Earths magnetic dipole inclination. 相似文献
12.
V. G. Vorobjev V. B. Belakhovsky O. I. Yagodkina V. K. Roldugin M. R. Hairston 《Geomagnetism and Aeronomy》2008,48(2):154-164
The optical observations on Heiss Island and the ion drift measurements on the DMSP F8 satellite were used to study the aurora characteristics and ionospheric convection before and after SC registered at 2330 UT on January 13, 1988. It has been indicated that two zones of luminosity can be distinguished in morning-time auroras during the quiet period before SC: the soft zone with auroral arcs and the harder diffuse auroral zone (equatorward of the first zone). After SC, a gradual smooth activation of auroras in both zones was followed (4–5 min later) by a more abrupt intensification of diffuse luminosity and by the appearance of numerous bright discrete auroras throughout the sky. In the diffuse auroral zone, the variations in the luminosity intensity with a period of 6–7 min were observed after SC. Auroral and geomagnetic field pulsations are closely correlated. During the quiet period before SC, sunward convection was concentrated in the soft precipitation region in the form of jets located in the vicinity of auroral arcs. After SC, considerable sunward convection was observed in the diffuse auroral zone. Peaks of the upward ion drift velocity were registered in the vicinity of auroral arcs. 相似文献
13.
极光卵极光强度的空间分布是太阳风-磁层-电离层能量耦合过程的重要表现,并且随着空间环境参数和地磁指数的变化而变化,是空间天气的重要指示器.建立合适的极光强度模型对亚暴的预测以及磁层动力学的研究具有重要意义.本文基于Polar卫星的紫外极光成像仪(Ultraviolet Imager,UVI)数据,采用两种不同的极光强度表征方法,即曲线拟合方法(从UVI图像数据中提取极光强度沿磁余纬方向上的曲线特征,Curve Feature along the Magnetic Co-latitude Direction of the Auroral Intensity,CFMCD_AI)和网格化方法(从UVI图像数据中提取极光强度的网格化特征,Gridding Feature of the Auroral Intensity,GF_AI),来构造极区极光强度特征数据库.然后,利用该数据库,采用广义回归神经网络(Generalized Regression Neural Network,GRNN)构建了以行星际/太阳风参数(行星际磁场三分量、太阳风速度和密度)和地磁指数(AE指数)为输入参数的两种极光强度预测模型(GRNN_CFMCD_AI模型和GRNN_GF_AI模型).利用图像质量评价指数结构相似度(structure similarity,SSIM)作为极光强度模型预测结果和对应的UVI图像的相似性评价标准(完全相似为1,不相似为0,一般认为SSIM大于0.5是具有较好的相似性),对两种极光强度模型进行了性能评价.结果显示,GRNN_GF_AI模型预测结果对应的SSIM值范围为0.36～0.77,均值为0.54,性能优于GRNN_CFMCD_AI模型的. 相似文献
14.
A. T. Kobea C. Amory-Mazaudier J. M. Do H. Lühr E. Houngninou J. Vassal E. Blanc J. J. Curto 《Annales Geophysicae》1998,16(6):698-710
Geomagnetic storm-time variations often occur coherently at high latitude and the day-side dip equator where they affect the normal eastward Sq field. This paper presents an analysis of ground magnetic field and ionospheric electrodynamic data related to the geomagnetic storm which occured on 27 May 1993 during the International Equatorial Electrojet Year (IEEY) experiment. This storm-signature analysis on the auroral, mid-latitude and equatorial ground field and ionospheric electrodynamic data leads to the identification of a sensitive response of the equatorial electrojet (EEJ) to large-scale auroral return current: this response consists in a change of the eastward electric field during the pre-sunrise hours (0400–0600 UT) coherently to the high-, mid-, and equatorial-latitude H decrease and the disappearance of the EEJ irregularities between the time-interval 0800–0950 UT. Subsequent to the change in hF during pre-sunrise hours, the observed foF2 increase revealed an enhancement of the equatorial ionization anomaly (EIA) caused by the high-latitude penetrating electric field. The strengthening of these irregularities attested by the Doppler frequency increase tracks the H component at the equator which undergoes a rapid increase around 0800 UT. The H variations observed at the equator are the sum of the following components: SR, DP, DR, DCF and DT. 相似文献
15.
A poleward-progressing 630 nm optical feature is observed between approximately 0100 UT and 0230 UT (0400 MLT to 0530 MLT) by a meridian-scanning photometer (MSP) located at Ny Alesund, Svalbard. Simultaneous coherent HF radar measurements indicate a region of poleward-expanding back-scatter with rapid sunward plasma flow velocity along the MSP meridian. Spatial maps of the backscatter indicate a stationary backscatter feature aligned obliquely with respect to the MSP meridian, which produces an impression of poleward-expansion as the MSP progresses to later MLT. Two interpretations of the observations are possible, depending on whether the arc system is considered to move (time-dependent) or to be stationary in time and apparent motion is produced as the MSP meridian rotates underneath it (time-independent). The first interpretation is as a poleward motion of an east-west aligned auroral arc. In this case the appearance of the region of backscatter is not associated with the optical feature, though the velocities within it are enhanced when the two are co-located. The second interpretation is as a polar arc or theta aurora, common features of the polar cap under the prevailing IMF northwards conditions. In this case the backscatter appears as an approximately 150 km wide region adjacent to the optical arc. In both interpretations the luminosity of the optical feature appears related to the magnitude of the plasma flow velocity. The optical features presented here do not generate appreciable HF coherent backscatter, and are only identifiable in the backscatter data as a modification of the flow by the arc electrodynamics. 相似文献
16.
D. G. Baishev E. S. Barkova A. E. Stepanov F. Rich K. Yumoto 《Geomagnetism and Aeronomy》2010,50(1):41-47
The synchronous observations of strong electric fields and large-scale undulations observed on December 12, 2004, in the evening
sector of the diffuse auroral zone 0900-1000 UT (~1700-1800 MLT) have been analyzed. The appearance of strong northward electric
field at ~0900 UT was almost simultaneously registered at Tixie Bay ionospheric station (71.6° N, 128.9° E, L =, 5.6) and on the DMSP F15 satellite. At 0910-1000 UT, the all-sky TV camera at Tixie Bay and the DMSP satellites (F13, F14,
and F15) registered eight undulations propagating westward at a velocity of 0.7—0.8 km/s. The undulation parameters registered
during the TV observations agree with the satellite measurements. The distinctive feature of the analyzed event consists in
that an intense electric field and undulations were localized within the diffuse zone in the region of increased precipitation
of keV electrons. A comparison of the ground-based and satellite measurements made it possible to draw the conclusion on the
necessary conditions for formation of diffuse undulations. 相似文献
17.
P.-L. Blelly J. Lilensten A. Robineau J. Fontanari D. Alcaydé 《Annales Geophysicae》1997,14(12):1375-1390
A set of EISCAT UHF and VHP observations is used for calibrating a coupled fluid-kinetic model of the ionosphere. The data gathered in the period 1200–2400 UT on 24 March 1995 had various intervals of interest for such a calibration. The magnetospheric activity was very low during the afternoon, allowing for a proper examination of a case of quiet ionospheric conditions. The radars entered the auroral oval just after 1900 UT: a series of dynamic events probably associated with rapidly moving auroral arcs was observed until after 2200 UT. No attempts were made to model the dynamical behaviour during the 1900–2200 UT period. In contrast, the period 2200–2400 UT was characterised by quite steady precipitation: this latter period was then chosen for calibrating the model during precipitation events. The adjustment of the model on the four primary parameters observed by the radars (namely the electron concentration and temperature and the ion temperature and velocity) needed external inputs (solar fluxes and magnetic activity index) and the adjustments of a neutral atmospheric model in order to reach a good agreement. It is shown that for the quiet ionosphere, only slight adjustments of the neutral atmosphere models are needed. In contrast, adjusting the observations during the precipitation event requires strong departures from the model, both for the atomic oxygen and hydrogen. However, it is argued that this could well be the result of inadequately representing the vibrational states of N2 during precipitation events, and that these factors have to be considered only as ad hoc corrections. 相似文献
18.
全天空极光成像仪是地基极光观测研究的重要仪器设备,从其拍摄的全天空图像数据中能获得极光形态、尺度、激发强度等重要物理参数,因而精确标定全天空图像,对准确获取极光相关物理参数极为重要.本文提出了一种基于星点位置信息对全天空图像进行标定的方法,通过该方法可以确定全天空图像参数(天顶在全天空图像中的像素点位置,地理方位以及视野范围内成像半径与天顶角的关系).利用电离层卫星探测到的极光沉降电子能谱中的"倒V"结构与极光弧之间的对应关系,对星点标定方法获取的全天空图像参数进行了验证.结果显示卫星穿越的"倒V"结构宽度(60±6km、102±6km)与同时全天空极光成像仪观测到的卫星穿越的极光弧宽度(64.7±7km、111.6±7km)几乎一致,这表明本文提出的全天空极光图像参数的星点标定方法是有效和准确的. 相似文献
19.
An intensification of auroral luminosity referred to as an auroral break-up often accompanies the onset of geomagnetic pulsation (Pi 2) at the dip-equator. One such auroral break-up occurred at 2239 UT on 16 June, 1986, being accompanied by weak substorm activity (AE≈50 nT) which was recorded in all-sky image of Syowa Station, Antarctica (66.2°S, 71.8°E in geomagnetic coordinates). The associated Pi 2 magnetic pulsation was detected by a fluxgate magnetometer in the afternoon sector at the dip-equator (Huancayo, Peru; 1.44°N, 355.9° in geomagnetic coordinates; 12.1°S, 75.2°W in geographic coordinates; L = 1.00). In spite of the large separation of the two stations in longitude and latitude, the auroral break-up and subsequent luminosity modulation were seen to be correlated with the wave form of the ground Pi 2 pulsation. This occurred in such a way that the luminosity maximum was seen to occur at the phase of maximum amplitudes of Pi 2 wave form. We argue that the observed correlation could be interpreted as indicating a Pi 2-modulation of a field-aligned acceleration of the low energy electrons that may occur near the equator of the midnight magnetosphere. 相似文献