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1.
收集广西北流5.2级地震序列波形和震相资料,采用结合波形互相关技术的双差定位方法对北流5.2级地震序列进行重新定位,采用CAP方法反演了北流5.2级地震震源机制。结合地质调查、地震烈度、地震精定位等结果,探讨了此次地震的发震构造。结果显示,北流5.2级地震序列呈北西向优势展布,震源深度主要集中在6~9 km。震源机制为走滑型,NWW向节面为可能的地震破裂面,初步推测NW向的米场-石窝断裂为发震断裂。  相似文献   

2.
采用地表地质调查、地貌调查、建筑物震害调查方法,结合震源机制解及余震分布、地震烈度图,初步探讨了广西北流M_S 5.2地震发震构造特征。研究结果表明:广西北流M_S 5.2地震发生在NW走向的石窝断裂和NE走向的新丰断裂交汇部位,发震构造为石窝断裂;石窝断裂露头平均产状222°∠81°,最新活动性质为具有正断分量的左行走滑断层,最新活动时代为早第四纪;新丰断裂最新运动性质为逆断,最新活动时代为早第四纪;在现今NW向主压应力作用下,石窝断裂发生破裂,发生M_S 5.2地震,同震运动方式以右行走滑为主,余震震中呈NW向分布。极震区建筑物震害调查得出的运动方向与震源机制解显示的同震运动方向一致。  相似文献   

3.
1999年岫岩地震序列研究   总被引:5,自引:0,他引:5  
用相对定位法对1999年11月29日辽宁省岫岩地区5.4级地震序列的前震、主震和余震进行了重新定位。结果是该序列的主震震源位置为40.538°N,123.026°E,深度为6.958km;重新定位的前震震中分布长短轴差别不大,分布在长轴约1.38km,短轴约1.23km,深度为6~11km的震源范围内,其中4级以上前震明显沿NW向分布,主震位于前震震中NW向分布的东南端;重新定位的余震明显沿NW走向分布,长轴约3.26km,短轴约0.79km,深度为5~12km,余震分布范围比前震分布范围大,主要是后期余震活动向SE向发展的结果。分析表明,1999年岫岩地震序列主要沿NW向分布,这个方向与1975年海城地震序列的NW向分布一致,与海城7.3级主震和岫岩5.4级主震震源机制解NW走向节面一致,也与海城 岫岩震区活动构造方向和岫岩主震的等震线长轴方向一致。并认为岫岩5.4级主震可能被前震触发,这为主破裂成核过程提供了一次实例。  相似文献   

4.
本文利用云南区域地震台网提供的震相报告,采用"多阶段定位"方法,对2021年5月21日云南漾濞Ms6.4地震序列的震源位置进行了重新定位.选取序列中13次具有高信噪比宽频带波形记录的Ms≥4.0地震事件,应用CAP波形反演方法,获取了这些事件的震源机制解和震源矩心深度.结果显示,漾濞地震序列震中距离NE侧的维西—乔后断裂约3~10 km,余震区长轴呈NW-SE向展布,长约22 km,震源优势分布深度为4~8 km,反映本次地震发生在上地壳浅部.地震分布北西窄、南东宽的分段特征明显,北西段地震更浅、更密集,南东段事件更深、更分散且存在向S偏转的现象.余震区不同位置的短轴剖面分析表明,发震构造倾向SW,南东段倾角缓于北西段.北西段还存在规模较小的NE向共轭断裂,长度约5 km.5月18日开始的前震自余震区中段向NW逐级迁移扩展,前震序列密集且存在相互触发,符合前震发生的级联模式.主震位于余震密集区的NW端,表明其具备SE向单侧破裂特征.多数4级以上地震的震源机制解都具有与序列长轴走向一致的NW-SE走向、高倾角SW倾向节面;基于震源机制解反演获得的区域构造应力场显示,发震构造受NNW-SSE向近水平主压应力作用发生右旋走滑运动,揭示主发震断层产状和错动类型与维西—乔后断裂基本一致.因此,可初步判定发震构造为维西—乔后断裂的平行伴生断裂,这一构造的形成可能与川滇块体SE向滑移和滇西南块体的顺时针旋转有关.  相似文献   

5.
2005年8月5日四川会东-云南会泽间5.3级地震序列初步研究   总被引:1,自引:0,他引:1  
2005年8月5日22时14分41秒,在四川省会东县与云南省会泽县交界一带发生了Ms5.3级地震。据西昌遥测地震台网测定:震中经纬度为26°35′N,103°03′E,震源深度为10千米。分析认为:这是一次前震—主震—余震型的地震序列事件。另外,由于这次地震情况比较复杂,根据周围20多个测震台站记录的P波初动解求解的震源机制解结果,初步认为这次地震的主震有可能是位于震区附近小江断裂带北段巧家—蒙姑断裂、蒙姑—东川断裂西侧北东向淌塘—岩坝断层北西上盘,在近水平的北北西向主压应力挤压作用下,发生了往北东方向逆冲的右旋错动的结果。  相似文献   

6.
利用来源于江西区域台网和中国地震台网共6个台的宽频带数字地震记录,采用CAP方法反演了2005年11月26日九江—瑞昌5.7级地震和4.8级强余震的震源机制解,并结合地震序列的精确定位结果和区域地质背景讨论了发震构造.结果显示,5.7级主震的最佳双力偶解为节面Ⅰ走向223°,倾角75°,滑动角144°;节面Ⅱ走向324°,倾角55°,滑动角18°.4.8级强余震的最佳双力偶解为节面Ⅰ走向54°,倾角71°,滑动角-160°;节面Ⅱ走向317°,倾角71°,滑动角-20°,这两次地震的震源机制解不完全一致.地震序列在震中空间分布和震源深度分布上也具有复杂性.5.7级主震发生后,余震活动从SE向NW、从浅部往深部发展,在破裂过程中可能遇到障碍体,触发了4.8级强余震.5.7级主震的发震构造可能为隐伏在瑞昌盆地内的洋鸡山—武山—通江岭NW向断裂,4.8级强余震的发震构造可能为瑞昌盆地西北缘的丁家山—桂林桥—武宁NE向断裂北段.  相似文献   

7.
在介绍盈江及邻近区域地震构造背景、新构造运动及区域构造应力场等的基础上,从2011年盈江5.8级地震烈度等震线、地震序列、地表形变带和震源机制解等方面,初步分析了本次地震的构造活动特征.结果显示,盈江5.8级主震与北东向大盈江断裂左旋走滑活动密切相关,前震和主震序列则反映出北东向大盈江断裂与近南北向苏典—盈江断裂共轭破裂活动的特征.通过区域历史地震概况和5.8级主震前后的地震活动情况,初步探讨了盈江地区的地震活动特点,认为群震是盈江地区地震活动的一大特点,5.8级地震的发生则是2011年年初4级群震继续增强活动的结果.  相似文献   

8.
2021年5月21日云南大理州漾濞县发生了MS6.4 地震.我们利用区域地震台网记录的地震波形资料,首先采用多点源地震矩张量反演方法确定了漾濞地震序列中 3 次MS≥5.0地震的矩心矩张量解,分析研究了地震矩释放的最佳模型;然后对序列中较大地震进行了绝对定位,结合余震序列重新定位结果研究了地震矩心在断层面上的位置.结果显示MS5.6 前震可用2 点源模型模拟,矩震级分别为MW 5.3、MW5.1,矩心时间相隔约30 s,矩心位置相距约 2 km.MS 6.4 主震可用单点源模型模拟,矩心与起始破裂点平面距离约 5 km.前震和主震的矩心均位于地表以下 6 km处,矩心与起始破裂点的位置关系显示两地震向南东方向单侧破裂,断层以"前震-主震"型地震序列典型的"撤退式"方式破裂,MS5.6 前震的发生降低了断层面的抗剪强度,从而发生了更大的MS6.4 主震.MS5.2余震可用单点源模型模拟,起始破裂点与矩心空间位置相近,在地表以下约 10 km处.余震区构造应力场反演结果显示漾濞 6.4级地震序列属于区域应力场触发的地震活动,地震序列震源机制解符合走滑断裂伴生的负花状构造系统内部断裂的运动特征,余震的空间分布图像显示花状构造系统内部的两条断裂发生了地震活动.  相似文献   

9.
利用理论波形与实际波形拟合方法 ,测定了发生于2019年10月12日22时55分26秒和24秒的广西北流-广东化州M_S5.2级地震(主震)及其M_L4.2级前震的矩震级,得到主震矩震级为M_W 4.7、前震矩震级为MW 4.2。  相似文献   

10.
利用来源于江西区域台网和中国地震台网共6个台的宽频带数字地震记录,采用CAP方法反演了2005年11月26日九江—瑞昌5.7级地震和4.8级强余震的震源机制解,并结合地震序列的精确定位结果和区域地质背景讨论了发震构造.结果显示,5.7级主震的最佳双力偶解为节面Ⅰ走向223°,倾角75°,滑动角144°;节面Ⅱ走向324°,倾角55°,滑动角18°.4.8级强余震的最佳双力偶解为节面Ⅰ走向54°,倾角71°,滑动角-160°;节面Ⅱ走向317°,倾角71°,滑动角-20°,这两次地震的震源机制解不完全一致.地震序列在震中空间分布和震源深度分布上也具有复杂性.5.7级主震发生后,余震活动从SE向NW、从浅部往深部发展,在破裂过程中可能遇到障碍体,触发了4.8级强余震.5.7级主震的发震构造可能为隐伏在瑞昌盆地内的洋鸡山—武山—通江岭NW向断裂,4.8级强余震的发震构造可能为瑞昌盆地西北缘的丁家山—桂林桥—武宁NE向断裂北段.  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.
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.
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.
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   

18.
Summary The maintenance of the axisymmetric component of the flow in the atmosphere is investigated by means of a steady-state, quasi-geostrophic formulation of the meteorological equations. It is shown that the meridional variations in the time-averaged axisymmetric variables can be expressed as the sum of three contributions, one being due to the eddy heat transport, another to the eddy momentum transport, and a third to the convective-radiative equilibrium temperature which enters the problem through the specification of a Newtonian form of diabatic heating. The contributions by the large scale eddies are evaluated through the use of observed values for the eddy heat and momentum transports.The contributions from each of the three forcing mechanisms to the temperature and zonal wind fields are invstigated individually and found to be of about equal importance. The sum of the three contributions are also presented for the temperature, the zonal wind, the stream function associated with the mean meridional circulation and the corresponding vertical motion. Although the results fail to reproduce the main observed features of the lower stratosphere, they are found to be in good agreement with observations in the middle latitude troposphere. At any pressure level, for example, the computed mean zonal wind has a jet-like profile and the axis of the jet is found to slope to the south with height, as observed in the atmosphere.Based in part on a thesis submitted by the first author as partial fulfillment of the requirements for the Ph.D. degree at the University of Michigan. — Publication No. 194 from the Department of Meteorology and Oceanography, The University of Michigan.  相似文献   

19.
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   

20.
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   

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