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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
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本文阐述了用１２０型非量测相机对南极中山站地区所摄制的１：４００００小象幅航片制作１：５０００地形图，正射像片图及１：１００００地形图的原理、方法和精度。在外定向中适当的权的情况下，其外定向最大对点误差平面为２．２ｍ，高程为１．２ｍ。所制作的正射像片图和相应的地形图套合中误差为０．１４４ｍｍ。 相似文献
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在南极中山站地区的土壤和湖泊沉积物中都有高岭石存在，本文分析了这些土壤样品的水溶态镁离子和ｐＨ值。结果表明，中山站地区土壤中的高岭石含量存在明显的空间分异，含量范围为２６％～５７％；而中山站地区奈拉湖不同时间的湖泊沉积物中高岭石含量范围则为５．８％～２３．２％。通过研究土壤中高岭石含量和土壤溶液性质的关系，发现土壤中高岭石含量与土壤溶液的ｐＨ和水溶态镁离子有一定联系。奈拉湖沉积物中高岭石的时间变化表明土壤中的高岭石含量在百年尺度上即可发生明显改变，这和土壤溶液性质发生改变的时间尺度是一致的。 相似文献
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本研究运用双频雷达(60MHz和179MHz)获取的南极中山站-Dome A断面的雷达回波探测数据,对冰盖浅部100-700m的雷达内部反射层和接收功率变化定量计算分析表明,60MHz的雷达回波能量比179MHz衰减得更快;中山站-Dome A断面冰盖浅层700m以上的雷达反射层形成的主导原因是冰密度的变化;断面上不同测站点间同一深度的接收功率差值达到10dB,表明冰盖浅层散射存在显著差异。 相似文献
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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
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利用南极长城站和中山站的降水、风、湿度、气压和云量等高质量的地面气象观测资料,对两站基本气候特征和变化趋势进行了分析。结果显示,长城站年降水量为503mm,年际变化呈减少趋势,变化速率为-27mm/10a。长城站和中山站年降水日数均呈下降趋势,变化速率分别为-2.9d/10a和-12.1d/10a。长城站和中山站年平均相对湿度分别为88%和58%。长城站年平均湿度总体上呈不明显下降趋势,中山站没有趋势。长城站盛行风向为西北风,中山站为偏东风,年平均风速分别为7.3m/s和7.1m/s。两站年平均风速呈减小趋势,变化速率分别为-0.09m/s/10a和-0.23m/s/10a。长城站平均大风日数为137d,记录的极大风速为37.2m/s。中山站平均大风日159d,记录的极大风速为50.3m/s。长城站和中山站年平均气压分别为990hPa和985hPa,变化速率分别为0.65hPa/10a和-0.80hPa/10a。其变化趋势相反,并与两站风速和大风日数及降水日数的变化倾向基本相同。长城站和中山站月平均云量分别为8.8和6.2,其差异显示了两站所处气候带的特点,即长城站地区全年阴天多、云量大,中山站则与此相反。 相似文献
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利用南极中山站和北极Tromso站1996、1997、1998及2002年的测高仪观测数据,对中山站(6月份)和Tromso站(12月份)上空冬季foF2的日变化特性进行了对比研究,结合数值模拟结果,分析了中山站和Tromso站F2层电离层的极区特征,进一步揭示了极区电离层特征的形成机理。结果表明,中山站和Tromso站虽然地理纬度接近,foF2日变化形成机理不完全相同。由于地磁纬度的差异,极区对流与日侧光致电离的相互作用造成了两站日侧电离层的不同变化形态,中山站foF2日变化主峰出现在磁地方时中午附近,而Tromso站foF2日变化主峰出现在地方时正午附近;两站日侧foF2受太阳辐射流量影响较大,极光沉降粒子电离在太阳活动低年对中山站foF2日变化形态影响显著。 相似文献
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利用我国最新地球重力场模型 WDM94,给出了南极 (纬度范围为 - 60°～ - 90°)大地水准面高和平均空间重力异常。为了全面总结分析南极大地水准面特征 ,收集了国外最新地球重力场模型 OSU91 ( 360阶次 )和 JGMOSU( 360阶次 ) ,计算了相应的大地水准面高和平均重力异常。其结果分别与 WDM94的结果作了比较 ,WDM94与 OSU91和 JGMOSU的大地水准面高标准差分别为± 1 .90 m和± 2 .0 9m,平均空间重力异常标准差分别为± 8.97mgal和± 9.32 mgal 相似文献
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The reduction of aliasing in gravity anomalies and geoid heights using digital terrain data 总被引：8，自引：0，他引：8
Observations of gravity can be aliased by virtue of the logistics involved in collecting these data in the field. For instance, gravity measurements are often made in more accessible lowland areas where there are roads and tracks, thus omitting areas of higher relief in between. The gravimetric determination of the geoid requires mean terrain-corrected free-air anomalies; however, anomalies based only on the observations in lowland regions are not necessarily representative of the true mean value over the topography. A five-stage approach is taken that uses a digital elevation model, which provides a more accurate representation of the topography than the gravity observation elevations, to reduce the unrepresentative sampling in the gravity observations. When using this approach with the Australian digital elevation model, the terrain-corrected free-air anomalies generated from the Australian gravity data base change by between 77.075 and −84.335 mgal (−0.193 mgal mean and 2.687 mgal standard deviation). Subsequent gravimetric geoid computations are used to illustrate the effect of aliasing in the Australian gravity data upon the geoid. The difference between 'aliased' and 'non-aliased' gravimetric geoid solutions varies by between 0.732 and −1.816 m (−0.058 m mean and 0.122 m standard deviation). Based on these conceptual arguments and numerical results, it is recommended that supplementary digital elevation information be included during the estimation of mean gravity anomalies prior to the computation of a gravimetric geoid model. 相似文献
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经1985年12月～1987年3月,三年度夏测绘科学考察,在中国南极长城站地区建立了一套完整的、精确的测绘基准系统。它包括大地坐标系统、高程系统和重力参考系统。本文叙述了建立这些基准系统的方法和数学模型,并分析了测量精度。 相似文献
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Takahito Kazama Hideaki Hayakawa Toshihiro Higashi Shingo Ohsono Shunsuke Iwanami Tomoko Hanyu Harumi Ohta Koichiro Doi Yuichi Aoyama Yoichi Fukuda Jun Nishijima Kazuo Shibuya 《Polar Science》2013,7(3-4):260-277
Absolute gravity values were measured with a portable absolute gravimeter A10 in East Antarctica, for the first time by the Japanese Antarctic Research Expedition. This study aims to investigate regional spatiotemporal variations of ice mass distributions and associated crustal deformations around Syowa Station by means of repeated absolute gravity measurements, and we obtained the first absolute gravity value in Southern Langhovde on the Antarctic Continent. The average absolute gravity value at the newly installed benchmark AGS01 in Langhovde (obtained on 3 February 2012) was 982535584.2 ± 0.7 μgal (1 [μgal] = 1 × 10?8 [m/s2]), which was in agreement with the gravity values obtained by the past relative gravity measurements within 1 mgal. In addition, the average absolute gravity value obtained at AGSaux in Syowa Station was consistent with both previous absolute gravity values and those obtained by simultaneous measurements using an FG5 gravimeter, owing to adequate data corrections associated with tidal effects and time variations in atomic clock frequencies. In order to detect the gravity changes associated with the ice mass changes and other tectonic phenomena, we plan to conduct absolute gravity measurements at AGS01 again and at other campaign sites around Syowa Station as well in the near future, with careful attention paid to the impacts of severe environmental conditions in Antarctica on gravity data collection. 相似文献
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Ottar Basin, SW Barents Sea: a major Upper Palaeozoic rift basin containing large volumes of deeply buried salt 总被引：1，自引：0，他引：1
Seismic mapping and gravity modelling of the Ottar Basin - a little studied Upper Palaeozoic graben in the south-western Barents Sea - demonstrates the presence of a major rift basin with large accumulations of unmobilized salt. Buried beneath thick, flat-lying Mesozoic strata, the NE-trending fault-bounded basin is at least 170 km long, varies in width between 50 and 80 km and coincides with a negative gravity anomaly of more than — 10 mgal. Seismic observations show that the south-western part is a half-graben tilted to the north-west whereas the north-eastern part appears to be more symmetric in shape. A large mass deficiency in the north-eastern part of the basin, indicated by a gravity anomaly of more than — 30 mgal, makes it necessary to postulate large amounts of salt within the basin. The preferred gravity model shows a total basin depth of 9.5 km, basin relief of 4.2 km and a salt volume of 6800 km3 corresponding to a 2.4-km-thick salt layer. Similar basin depths, but only 500–600 km3 of salt, are indicated beneath the Samson Dome in the south-western part of the basin. Unlike salt bodies in other Barents Sea basins, the thick salt deposit in the north-eastern part of the Ottar Basin is relatively unaffected by halokinesis. Interfingering of different basin facies, lack of tectonic reactivation of the basin and a relatively late differential loading by protruding cover strata probably explain these differences in development. The large size and voluminous salt deposits establish the Ottar Basin as one of the major Barents Sea evaporite basins and an important structural component of the Upper Palaeozoic rift system. 相似文献
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以往对"三驾马车"认知停留在其对经济增长的增量影响,缺乏空间方向概念。由此,以经济重心作为衡量经济空间结构的指标,并以广西为例,从拉动经济增长的消费、投资和出口"三驾马车"视角出发,通过重心和灰色关联度模型,对比分析"三驾马车"重心与经济重心的演化路径,进一步揭示三大拉力对经济重心空间迁移的影响。结果表明:2004—2014年广西经济重心迁移路径呈"S"型,2010,2013年分别为重心空间转向的拐点;在空间位置方面,与经济重心邻近程度由高至低依次是消费重心、投资重心和出口重心;在迁移路径方面,消费重心的移动距离最小且变动较为稳定;出口重心的移动距离最大,整体上呈往西南方向迁移态势;投资重心与经济重心的迁移路径在2009年以后的走势较为一致。在拉力作用方面,"三驾马车"对经济重心在不同阶段及不同方向上的影响强弱不一,整体而言是投资大于消费大于出口。 相似文献
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在山区 ,尤其是在有全球第三极之称的喜马拉雅山区 ,当相邻点间距不大时 ,如何利用这些点上的重力与地形 (高程 )数据推估待求点的重力值 ,这对难以攀登和不能用仪器观测的山峰很有意义。研究指出 ,在地形负荷的波长很短时 ,具有一定强度的地壳足以能够支撑这种负荷 ,因此 ,不能用Airy Heiskanen和Pratt Hayford局部补偿模型作重力推估 ;由于空间异常主要受地形起伏制约 ,因此借助于邻近重力点的地形 (高程 )作推估会得到满意的结果。基于这一思路 ,我们采用了 4种有关公式 ,有效地推估了第三极之巅珠穆朗玛峰顶上的重力值 ,该值为(976 970± 7)× 1 0 - 5m·s- 2 。这一结果为精确推求珠峰大地水准面和正高提供了必要的数据 ,若用均衡的方法来推估 ,则可能相差近 1 0 0× 1 0 - 5m·s- 2 。 相似文献