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1.
刘长发  张平 《南极研究》1996,8(3):54-60
利用南极地磁资料研究了地磁扰日变化SD场特征。1.SD场变化不如Sq场变化规则,无明显的昼夜差异;太阳活动高年比下降年SD场变化更强烈。2.极隙区中山站SD场变幅比亚极光区长城站和北半球低纬区北京台的SD场变幅大10倍以上。3.中山站S^-D变化呈“正弦波”形态,与长城站和北京台S^-D变化形态相反。4.中山站S^-D等效电流矢量在早晨-下午矢量方向为反时针西向,下午-夜音矢量方向为顺时针东向,这  相似文献   

2.
王英鉴 《南极研究》1995,7(2):45-50
利用可见/紫外差分吸收光谱学方法,在1991年南极臭氧洞期间对中山站地区的大气臭氧和NO2含量进行了测量。分析结果指出,对中山站地区面言,1991年大气臭氧含量的迅速减少开始于8月中旬,到10月3日达最低值,并很于10月7日恢复到正常值。  相似文献   

3.
南极中山站固体潮观测分析   总被引:3,自引:0,他引:3  
郝兴华  许厚泽 《南极研究》1995,7(3):109-112
中国南极中山站位于南极拉斯曼丘陵地区,1991年3月至1993年2月,用Lacoste ET型重力仪,在这个地区进行了为斯的两年的观测,取得了600多天有效资料,经调和分析和流变模型,海潮负荷必正后得到:δol=1.2253±0.0031,Δψol=0.73°±0.14°;δm2=1.0785±0.0045,Δψm2=-3.55°±0.29°从资料分析的精度来看,观测资料是比较好的;但由于海潮负荷  相似文献   

4.
本文了分析1991年太阳活动峰年南极中山站地磁静日Sq变化,结果表明:1)地磁静日Sq变化叠加很多扰动。Sq场是由S0q场和Spq场所组成。2)Sop场变化比较规则,其极昼月的变幅比极夜月大很多。在极昼月S0q(H)变化出现有双峰图象。Sop场主要是由高结局度极区电离层Sq电流体系所控制。  相似文献   

5.
南极臭氧洞期间中山站和昭和站大气臭氧的中期振荡特征   总被引:1,自引:0,他引:1  
本文用1993和1994年7-12月中山及昭和站大气臭氧观测资料和1993年7-12月中山站地面温度,气压及戴维斯站探空资料,对南极臭氧洞期间中山站和昭和站的中斯振荡特征进行了研究。结果表明:准一周和准二周振荡是南极地区大气臭氧和各层次温压参数普遍存在的两种主振荡周期,且在不同年份其振荡强度也有所不同。  相似文献   

6.
王英鉴 《极地研究》1995,7(2):48-53
利用可见/紫外差分吸收光谱学方法,在1991年南极臭氧洞期间对中山站地区的大气臭氧和NO2含量进行了测量。分析结果指出,对中山站地区而言,1991年大气臭氧含量的迅速减少开始于8月中旬,到10月3日达最低值,并很快于10月7日恢复到正常值。大气臭氧和NO2的变化有很好的正相关性,相关系数达0.69;臭氧洞期间,NO2含量一直处于低值,且层的高度较高。这表明1991年春季中山站地区臭氧含量的减少不是由奇氮的的催化损耗过程所致  相似文献   

7.
中国南极中山站位于南极拉斯曼丘陵地区(λ=76°22′E,φ=69°22′S),1991年3月至1993年2月,用LacosteET型重力仪,在这个地区进行了为期近两年的观测,取得了600多天的有效资料,经调和分析和流变模型、海潮负荷改正后得到:δo1=1.2253±0.0031,Δφo1=0.73°±0.14°;δm2=1.0785±0.0045,Δφm2=-3.55°±0.29°从资料分析的精度来看,观测资料是比较好的;但由于海潮负荷改正缺少附近海域的资料,会对最终结果造成较大的影响  相似文献   

8.
南极中山站NO_2的观测及平流层NO_2与O_3的关系分析   总被引:6,自引:0,他引:6       下载免费PDF全文
利用Brewer臭氧仪对南极中山站上空的O3、NO2柱总量及平流层O3、NO2含量进行了长期观测研究,分析了1993~1995年,尤其是1995年南极臭氧洞和非臭氧洞时期NO2柱总量及平流层NO2含量的季节变化及与O3含量的关系,指出平流层NO2含量的减少是造成南极臭氧洞成因和近年来不断加剧的一个主要原因。  相似文献   

9.
杨少峰 《极地研究》1992,4(1):42-50
本文将我国首次南极考察得到的长城站地磁脉动资料与北京地区的同时地磁脉动观测资料作比较。对比分析表明 ,在磁静日中两个地区以平静的脉动为主 ,南极长城站有时出现Pc1 /Pc4- 5脉动 ,北京地区会出现 Pc3脉动。Pi脉动出现很少。但在磁扰日中 Pi型脉动出现次数明显增加 ,还会出现在对应的小时段上。不过长城站的 Pi脉动往往比北京地区强些。  相似文献   

10.
基于南极中山站数字式电离层测高仪DPS-4D和GPS-TEC电离层闪烁监测仪的观测数据,比较研究了两者在2013年所得电离层总电子含量(TEC)随太阳辐射和地磁活动的日变化和季节变化特征。比较结果表明,南极中山站上空电离层TEC存在明显的极区电离层变化特性,这种变化特性大体与太阳辐射成正相关关系,而与地磁活动成负相关。尽管电离层TEC变化具有明显的晨昏不对称性,但都能有效地被DPS-4D和GPS TEC监测仪的数据计算获得,且两者相关系数达到0.86。结合中山站所处的极区电离层位置,考虑太阳辐射电离和地磁活动影响下的极区电离层对流以及中性大气成分改变,初步分析了DPS和GPS所得TEC结果有所差异的原因。  相似文献   

11.
杨少峰  刘勇华 《极地研究》1999,10(2):155-162
In this paper the data of geomagnetic pulsations at Zhongshan Station from February 3 to Novernber 30 in 1996 are analyzed in ordcr to study polarization characteristics of Zhongshan Station Pc3 pulsations which comprises the cusp Pc3 pulsation and the nightside Pc3 pulsation. For the cusp Pc3 pulsation. the right-handed polarization is always dominant. But their orientation of major axes of polarizations changes with season, NW-SE is dominant in summer and NE-SW in winter. For the nightside Pc3 pulsation,the right-handed with NE-SW is always dominant before midnight. But the left-handed with the mixing orientation of major axes is dominant in summer and the NE-SW with the mixing polarization sense is dominant in winter after midnight. It means that the two types of Zongshan Station Pc3 pulsations have different sources.  相似文献   

12.
利用南极地磁资料研究了地磁扰日变化SD场特征。1)SD场变化不如Sq场变化规则,无明显的昼夜差异;太阳活动高年(1991年)比下降年(1994年)SD场变化更强烈。2)极隙区中山站SD场变幅比亚极光区长城站和北半球低纬区北京台的SD场变幅大10倍以上。3)中山站S0D(H)变化呈“正弦波”形态,与长城站和北京台S0D(H)变化形态相反。4)中山站S0D等效电流矢量在早晨-下午(02~15h)矢量方向为反时针西向,下午-夜间(15~02h)矢量方向为顺时针东向,这是由极区东向、西向电射流和极区电流涡旋所引起;长城站与北京台S0D等效电流矢量很小,这是由极区东向和西向电射流的影响所致。  相似文献   

13.
在南极中山站使用TD-4A测高仪,从1990年3月至今已取得了10万余帧的电离图记录。由于中山站处在极尖区附近这样一个特殊位置,所以这些电离图能显示出大多数高纬现象,诸如极光卵现象、FLIZ(F层不均匀区)现象、倾斜Es和空白现象、F区磁纬中午现象、E和D区的粒子沉降效应,以及粒子E层(夜间E层)现象等。本文对这些现象进行了描述和初步分析。  相似文献   

14.
中国极区高空大气物理学观测研究进展   总被引:3,自引:0,他引:3       下载免费PDF全文
刘瑞源  杨惠根 《极地研究》2011,23(4):241-258
中国南极长城站、中山站、昆仑站和北极黄河站有着独特的地理位置,非常适合于开展极区高空大气物理学的观测研究.回顾中国极地考察研究近30年历程,综述极区高空大气物理学研究方面取得的主要进展,他们是:在南极中山站和北极黄河站建立了国际先进的极区高空大气物理共轭观测系统,实现了极区空间环境的连续监测;在极区电离层、极光和粒子沉...  相似文献   

15.
《极地研究》2002,13(1):55-66
In this article we want to present the EISCAT Svalbard Radar (ESR) in some detail, as well as some of the instruments of interest for ionospheric and magnetospheric research that are located in the vicinity of it. We particularly describe how this instrument cluster, close to the geomagnetic conjugate point of the Chinese Antarctic Zhongshan Station, can contribute to inter hemispheric coordinated studies of the polar ionosphere.  相似文献   

16.
Two induction magnetometers have been installed at Chinese Zhongshan Station and Australia Davis Station, Antarctica respectively. We adopt the cross spectral analysis technique to analyze the data of the two induction magnetometers, in June, September, December 1996 and March 1997, and to investigate Pc5 frequency range pulsation (150 600 s) occurrence and propagation in cusp latitude. The results are summarized as follows: At Zhongshan Davis Station, the magnetic pulsations in Pc5 frequency band can occurs over a wide time, but more frequently at pre local magnetic noon and pre local magnetic midnight. The Pc5 pulsations have no significant seasonal variation in the amplitude, occurrence and propagation. The amplitude has a small peak at pre local magnetic noon and large value sometimes at pre local magnetic midnight. In daytime, the Pc5 pulsations propagate westward in morning and eastward in afternoon, and reversal at local magnetic noon. In nighttime, the Pc5 pulsations propagate westward before 20:00 MLT and eastward after 20:00 MLT. Near dusk time, the Pc5 pulsations propagate irregularly. These characteristics indicate that the Pc5 pulsations have different source at different local magnetic time.  相似文献   

17.
In this paper Pi2 pulsations at Zhongshan Station of Antarctica are analyzed from October 1 - 31, 1996. Their characteristics e. g. occurrence frequency,frequency, and polarization are studied. The characteristics of Pi2 pulsations are summerized as follows: (1 ) Pi2 pulsations at Zhongshan Station usually take place from 2000 MLT to 0200 MLT; the main frequencies are between 6. 79 mHz and 13. 58mHZ; (2 ) Pi2 pulsations with low frequencies are dominent. The range of main frequencies becomes narrow at midnight; (3) The Polarization of Pi2 pulsations are almost linear; (4) About the orientation of major axes the NW-SE direction is dominent before 2200 MLT and NE-SW is dominent after 2200 MLT. The generation mechanism of Pi2 pulsations at Zhongshan Station is discussed theoretically.  相似文献   

18.
Two induction magnetometers have been installed at Zhongshan Station and Davis Station, Antarctica respectively. We adopt with cross-spectral analysis technique to analyze the data of the two induction magnetometers, in June, September,December 1996 and March 1997. to investigate the Pc3 frequency range pulsation occurrence and propagation characteristics in the cusp latitudes. The results are summarized as following:At Zhongshan-Davis Stations, the Pc3 frequency range pulsations occur mainly around the local noon/ local magnetic noon and local magnetic midnight respectively. In daytime, the pulsations have a seasonal variation in amplitude, occurrence and temporal range, all of them are sma1lest in winter. But in nighttime, the pulsations have no such a variation. The pu1sation amplitude in nighttime is much larger than the one in daytime all oveI the year. The pulsation propagating direction is mainly western in daytime and irregularly in nighttime. It can be thought that the different sources of the pulsation and the ionospheric electric conductivity are mainly responsible for these characteristics.  相似文献   

19.
Based on data of Digisonde Portable Sounder-4 (DPS-4 ) in 1995 -1997. we have analyzed the seasonal variations of F region at Zhongshan Station (69. 4°S,76. 4°E ). During the summer of Zhongshan Station, F region ionization is mainly controlled by the solar ultraviolet radiation. Similar to the phenomena in mid-latitude area, the value f0F2 is changed with local time. During equinox scasons, soft electron precipitation from the cusp/cleft region seems significant, f0F2 is changed with rnagnetic local time, and shows the magnetic noon phenomenon. In winter. the effect of the solar radiation on the F region is less than that of summer. Instead, F region is affected by particle precipitation from cusp/cleft region as well as polar plasma convection, there fore, the diurnal variation of f0F2 is more complex and shows two peaks. F region occurs all day in summer. and seldom appears at midnight in equinox.In winter, F region shows two minimums, one is at midnight and the other is at afternoon cusp. Further analysis of the F region spread indicates that in winter the aurora oval passes over the Zhongshan Station is at 1100 UT - 1500 UT.  相似文献   

20.
2000年7月重大太阳事件的极隙区纬度观测研究   总被引:4,自引:0,他引:4       下载免费PDF全文
20 0 0年 7月 ,太阳表面发生了一系列的耀斑与日冕物质抛射事件 ,最大耀斑能级达X5 .7/3 B。地球表面发生相应特大磁暴 ,Dst指数最大负偏达 - 3 0 0 n T。中国南极中山站地处极隙区纬度 ,白天位于磁层极隙区 ,夜间位于极盖区 ,以多种高空大气物理观测设备详细记录了该磁暴过程。对有关数据的分析表明 ,高能粒子引起电离层吸收急剧增加 ,测高仪数据两天多信号空白 ,宇宙噪声吸收显著增加 ;地磁 Pc3 /5脉动增加与行星际磁场南向分量密切对应 ,显示行星际磁流体波对激发磁层脉动的贡献 ;磁暴主相期间 ,Pc3 /5脉动大幅度增加 ;极区地磁水平分量随南向行星际磁场变化 ,但滞后近 8小时 ;Dst指数与南向行星际磁场密切相关 ,磁暴受控于高度负偏的南向行星际磁场  相似文献   

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