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1.
和田地震台地倾斜观测资料某些震例分析 总被引：1，自引：0，他引：1
1 台站情况简介和田地处北北东向阿尔金断裂带和东西向西昆仑山前断裂带的交汇部位 ,是地震多发地区之一。本世纪以来 ,该区发生 6级以上的地震 8次 ,5.0～ 5.9级地震 2 3次 ,地震活动相当频繁。和田地震台建于 1 979年 ,1 980年开始使用金属摆倾斜仪进行地倾斜观测 ,至今已有 2 0多年的连续观测资料。其观测值存在明显的趋势变化背景和较好的年变形态 ,在大潮时能记录到清晰的固体潮形态。地倾斜仪安装在 8m深的地下室 ,该观测室顶部覆盖约 3 m,台基岩性为第四纪松散沉积物。地下室内年温差约 5℃ ,日温差小于 0 .1℃ ,湿度小于 50 %。仪… 相似文献
2.
宁蒗-盐源地震前的西昌地磁短临异常特征 总被引：2，自引：0，他引：2
1 西昌地磁台基本情况简介 西昌地磁台位于西昌市西郊的泸山园艺场内,距市中区5 km.占地面积约200 m2属国家二类基本地磁台.台址位于川滇棱形块体的安宁河断裂东面,紧靠则木河断裂西侧,属第四纪冲积、坡积带.土壤层大部为坚硬板土和昔格达砾岩,无明显磁性.室内外磁场总强度水平梯度一般小于5 nT/m.仪器观测室和记录室均采用无磁性或弱磁性灰沙砖、木结构材料建筑.室内全年最低温度11.5 ℃,最高28.1 ℃.日温差一般小于0.3 ℃,最大周日变化均为0.5 ℃.相对温度小于80%.现有投测于1986年的绝对观测CJ6地磁经纬仪两台(水平度盘最小刻度1′),投测于1958年的CZM-2质子旋进式分量仪一台(最小读数1 nT);投测于1985年的CB3地磁记录仪两台(标度值相对误差＜1.5%). 相似文献
3.
本文测定了中国西北六省地区Lg 波的传播速度,V_(Ig)=3. 56km/s;并测得了该区约1秒Lg 波的滞弹性衰减系数,r=0. 0021±0. 0002km~(-1) ,相当于介质品质因子Q=599±56。建立了该区m_(Lg)震级公式m_(Lg)(m×h)=1gA_(m×h)+q_(NW)(Δ)+Dh其中震级校准函数q_(NW)(Δ)=(5/6) 1g△+0. 00091Δ+1. 88 相似文献
4.
富蕴台地倾斜异常与斋桑泊7.3级地震 总被引：1，自引：0，他引：1
富蕴台倾斜资料异常及预报意见 富蕴地震台位于我国新疆东北部阿勒泰地区。倾斜仪安装在浅山洞进行观测,山洞进深12.3m,覆盖厚度11m,基岩性质为石英岩,仪器墩为水泥、石块浇灌而成。1990年洞室年温差4.3℃,日温差0-0.1℃,使用JB型金属水平摆倾斜仪观测,光杆距2m,工作格值0.008/mm。 该台站自1976年开始地倾斜观测,1982年8月中断,1985年2月恢复观测。平静时期资料的变化比较正常稳定,年变化规律比较清楚,图1给出了1985年恢复观测以来富蕴台地倾斜月均值矢量合 相似文献
5.
2003年2月14日01时32分、01时34分,距石场台站13km、26km处相继发生两次5.0和5.4级中强地震(φN43°59′;λE85°51′);(φN44°00′;λE85°52′)。这是建台以来震中离台站最近、强度最高、震感最为强烈的两次地震。利用地形变学科分析预报方法对以上两次地震的单台资料进行综合分析,及时捕捉震前短临异常信息,为预测本监视区未来地震提供了依据。1 观测点概况石场地震台SQ-70型石英摆式倾斜仪架设在台站以南2km处的山洞内。山洞进深18m,台基为侏罗纪砂岩,覆盖厚度约30m,年温差小于2℃。1989年对山洞进行保温改造后仪器连续工作至今(… 相似文献
6.
德都地磁台始建于1976年,用于安装地磁记录仪的记录室是北方台站中唯一的一个纯地上建筑,很难达到《地磁台站观测规范》中对地磁记录室要求的日温差≤0．3℃、年温差≤20℃,特殊地区不大于30℃的标准,特别是最近几年,由于房屋墙体的保温材料下沉,使保温层出现裂缝,造成记录室的日温差、年温差在温度变化明显的季节,都严重超差,从而严重影响本地震台水平分量、垂直分量的基线值精度。为此,我们研制了CB-3磁变仪的温度控制系统(国家地震局,1990;中国地震局,2001)。 相似文献
7.
本文基于1987—2017年南极点的无线电探空数据,研究了地面至30 km海拔高度的气温、风向和风速的垂直分布及变化趋势.多年平均的逐月数据表明,气温在各高度上均具有显著的季节变化,南半球夏季（冬季）对流层低层温度最高达-25℃（最低达-60℃）,分别出现于1月（7月）地面以上约500 m（近地面）.近30年来,年平均地面气温呈0.3℃/10a的增加趋势,增温趋势总体上随高度增加而减缓,至对流层上层的气温变化趋势为负,约为-0.25℃/10a.对于对流层整层平均气温,秋季上升趋势在四季中最为明显,达0.55℃/10a,而年平均气温的趋势约为0.3℃/10a.近地面全年盛行东北风,风速大多在2~10 m·s-1范围内;对流层的低层（高层）为西北风（西南风）,在海拔6~9 km处,对流层急流可达25 m·s-1;而平流层低层（高层）为南风（东南风）,最大风速可超过30 m·s-1.风速和温度梯度变化特征在地面至10 km（10~30 km）高度段表现为负相关（正相关）.近30年近地面呈现北风增加东风减少的趋势,而高空南风减少,东风和北风增多.对流层整层平均风速显示,各季节平均风速均呈增加趋势,并且与温度类似,秋季的增加趋势最显著,达0.59 m·s-1/10a,而春季趋势最为平缓,仅0.05 m·s-1/10a.对流层整层年平均风速的线性趋势为0.24 m·s-1/10a,地面年平均风速呈0.05 m·s-1/10a的增加趋势. 相似文献
8.
前言长春合隆地震台是中国地震局 类基本地磁台 ,正式出版的地磁观测报告及磁暴报告与 4 0多个国家 (或地区 )实行资料交换。1 981年 ,台站投入形变电阻率 (简称地电 )观测 ,设置 N4 5°E,N4 5°W两测道 ,为十字型对称性布极 ,供电极 ( A、 B)极距为 2 0 0 0 m,1 992年改为 1 3 0 0 m,测量极 ( M、 N)极距为 4 0 0 m。观测中心点位于地磁观测室南 1 70 m处 ,供电线 ( A1 B1 )在地磁观测室及记录室西侧 ,垂直距离 1 50 m;供电线 ( A2 B2 )在地磁观测室及记录室东侧 ,垂直距离 1 1 0 m。地电观测证明 ,向 A、 B电极供电时 (直流 2 .4 A… 相似文献
9.
据中国地震台网测定 ,2 0 0 1年 1 1月 1 4日1 7时 2 6分 (北京时间 )在新疆 -青海交界一带( 3 6.2°N,90 .9°E)发生了 MS8.1大震。地震使青海震中区部分房屋倒塌 ,青藏公路 (国道1 0 9线 )多处断裂 ,昆仑山出现一条大裂缝带 ,正在施工中的青藏铁路格拉段受到破坏。我们利用 CDSN的 7个台站的数字波形资料初步反演了该地震的震源参数 ,结果如下 :最佳双力偶解 : Strike Dip RakeNP1 :0° 46° 1 49°NP2 :1 1 3° 68° 49°应力轴 : Val Azm PlgT: 2 .5× 1 0 2 73 3 8° 49°N: -0 .9× 1 0 … 相似文献
10.
根据苏北测震台网地面台站和深井台站记录的地震波形资料,分析2009年10月以来台网附近 ML ≥2．8地震波频谱特性。分析可知：地面记录与井下记录的地震波频谱特性存在一定差异,地面记录地震波拐角频率较井下约大0．28 Hz,地震波峰值频率比井下约小0．22 Hz;对于ML ＞4．5地震,地面记录地震波的优势频率范围小于井下记录;地震矩和矩震级地面台站记录数值较大,差值分别为3．104×10^14 N·m 和0．32级。 相似文献
11.
12.
The determination of the coefficient of viscosity of eruptive products gives useful elements to the knowledge of possible variations of composition and physical conditions of the magmas. 相似文献
13.
Studia Geophysica et Geodaetica - 相似文献
14.
Geomagnetism and Aeronomy - The magnetic evolution of the active region of the Sun at the level of the photosphere has been studied. Magnetic synoptic maps of the 2007 Kitt Peak Observatory were... 相似文献
15.
V. E. Pavlov T. Yu. Tolmacheva R. V. Veselovskiy A. V. Latyshev A. M. Fetisova I. V. Bigun 《Izvestiya Physics of the Solid Earth》2017,53(5):702-713
Until recently, the existing data prevented the geophysicists from accurately dating the Bysy-Yuryakh stratum, which outcrops in the middle reach of the Kotuy River, constraining the time of its formation to a wide interval from the end of the Late Cambrian to the beginning of the Silurian. The obtained paleomagnetic data unambiguously correlate the Bysy-Yuryakh stratum to the Nyaian regional stage and constrain its formation, at least a considerable part of it, by the Tremadocian. This result perfectly agrees with the data on the Bysy-Yuryakh conodonts studied in this work and yields a spectacular example of the successful application of paleomagnetic studies in solving important tasks of stratigraphy and, correspondingly, petroleum geology. Within the Bysy-Yuryakh stratum, we revealed a large normal-polarity interval corresponding to the long (>1 Ma) period when the geomagnetic reversals were absent. This result, in combination with the data for the Tremadocian and Middle–Upper Cambrian sequences of the other regions, indicates that (1) the rate of occurrence of the geomagnetic reversals on the eve of the Ordovician Moyero superchron of reversed polarity was at most one reversal per Ma; (2) the superchron does not switch on instantaneously but is preceded by a certain gradual change in the operation conditions of the dynamo mechanism which, inter alia, manifests itself by the reduction of the frequency of geomagnetic reversals with the approach of the superchron. This finding supports the views according to which a process preparing the establishment of the superchrons takes place at the core–mantle boundary. 相似文献
16.
Summary A simple model is proposed suitable for studying the effect of the ground layer of the atmosphere, polluted by aerosol, on the albedo. This model is founded on solving the equation of transfer of radiative energy. The numerical results are discussed, particular attention being paid to the analysis of errors due to neglecting the multiple reflection of solar radiation on the aerosol particles. A method which would also include the multiple reflection is proposed, and the conditions under which the presence of the aerosol is responsible for an increase or decrease of the solar radiation balance on the Earth's surface, are analysed. 相似文献
17.
Josef Vykutil 《Studia Geophysica et Geodaetica》1968,12(2):217-220
Резюме Дается вывод формул для вычислений длины хорды, длины и азимутов нормаляных сечений и длины геодезической линии эллипсоида.
Применяются тригонометрические функции данных величин и постоянные принятого ргфгргнц-эллипсоида, что является целесообразным
при использовании вычислителQjных машин, особенно автоматов. Рабочие формулы рекомендуются в форме (8–11).
Dedicated to Professor František Fiala on His 85th Birthday
Address: Veveři 95, Brno. 相似文献
Dedicated to Professor František Fiala on His 85th Birthday
Address: Veveři 95, Brno. 相似文献
18.
Ivanka Jakubcová Věra Marvanová Miloš Pick Antonín Novotný Reviewer Z. Šimon 《Studia Geophysica et Geodaetica》1982,26(2):193-196
Summary The results of two different methods of the determination of the non-linearity of the gravimeter scale are compared; the economy is discussed as well. 相似文献
19.
Atmospheric temperature and humidity fields as well as information on other meteorological parameters are nowadays retrieved from radiance measurements recorded by operational meteorological satellites. Up to now, the inversion procedures used only take into account crude information on the topography of the Earth’s surface. However, the applied radiative transfer codes have to consider the Earth’s surface as the lower boundary of the atmospheric model and, therefore, need a more precise mean elevation and a classification of the roughness of the Earth’s surface. The influence of the topography of the Earth surface on retrieved temperature profiles is studied by using a physico-statistical inversion method. An objective analysis is made of the more precise mean elevation and derivation of roughness parameters using a new high-resolution digital elevation model (DEM) with a resolution of 500 m×500 m. By means of a geomorphological process and a newly developed topography rejection test, areas with a high surface roughness are localized and singled out. The influence of topography on the retrieved temperature profiles is illustrated by case studies. Changes are found predominantly in areas with a high variation of topography. Using the new high-resolution DEM and the topography rejection test, the geographical position of the calculated temperature profiles tends to be shifted towards areas with a small vertical variation of topography. The mean elevation determined by the new elevation model better characterizes the area observed. Hence, the temperature profiles can be calculated down to lower atmospheric levels. Furthermore, a guess profile better describing the atmospheric situation is selected by the more precise elevation. In addition, the temperature profiles obtained near the coast are improved considerably by the more precise determination of the surface property ‘sea’ and ‘land,’ respectively. Integration of an independent physical information such as topography leads, on average, to a slight improvement of the results of the physico-statistical inversion procedure. In some cases, however, significant improvements have been achieved regarding the desired accuracy of temperature profiles of the order of 1 K. In future, the spatial resolution of new high-resolution sounding instrumentation on the next generation of operational meteorological satellites will be increased. To exploit the resolving power of this new instrumentation, the different variation of the topography of the Earth surface, especially in regions with a high variation of topography, can be taken into account more precisely by using a high-resolution DEM. 相似文献
20.
Prof. Dr. W. A. Heiskanen 《Pure and Applied Geophysics》1958,41(1):1-18
Summary The author mentions the aims of the World-wide gravity project he established in the Ohio State University in Columbus, in 1950. He outlines the practical procedure of the gravimetric computations of the undulationsN and the vertical deflection components and and emphasizes that only by the global international cooperation and additional gravity observations at sea carried out during the last decade it has been possible to gather to Columbus the needed gravity material. Since there exist still large gravimetrically unsurveyed areas it is of vital significance to study what gravity anomalies are best to be used for these regions. The given figures concerning the accuracy of theN, and , estimated theoretically and obtained in practice, indicate that in the gravimetrically well surveyed parts of the world like in Europe and the United States we can get gravimetrically on basis of existing gravity material theN-values with accuracy of about 5–10 meters, and and with the accuracy of about 1. The geoid undulationsN are already computed in Columbus for more than 6000 points of the northern hemisphere. The sample maps show the interesting geoid of Europe and vicinity between the latitudes 60° and 30° and longitude 5° W and 30° E, drafted on basis of more than 1000N-values computed at the corners of 1°×1° squares. It is interesting to realize that the geoid undulations in all this area are positive, the extreme values being between 40 and 50 meters. The geophysical significance of the geoid maps of this kind is pointed out. 相似文献