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1.
结合使用人工地震折射测线和天然地震观测资料，给出了龙门山断裂带P波和S波的地壳平均速度模型．以此模型为基础，修定了沿龙门山断裂带分布的202个地震，给出了震源位置误差小于1.5 km的精确解．以到时曲线为准，将修定后的震源参数与四川台网常规定位的震源参数进行了比较，到时数据相对于时距曲线极小的分散，证明定位后的震源位置的精度得到了相当的改善．所获得的震源分布表明，地震活动主要发生在沿龙门山主中央断裂．绝大多数地震分布在3～22 km深度范围的上地壳中．结果证明，本文所提供的速度模型和采用的定位方法是适合龙门山断裂带地震定位使用的；配合日本东北大学提供的实时处理系统，对提高四川台网的定位精度是十分有效的． 相似文献
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2008年5月12日四川龙门山断裂带发生了汶川8.0级地震,之后四川境内发生了两次7.0级地震(其中一个是芦山地震),为了研究汶川地震之后龙门山断裂带及周边区域的地震活动性,本研究收集了国家地震台网和四川区域地震台网2010年1月1日—2017年12月31日四川地区发生的17次M≥5.0地震以及120多次5.0>M≥4.0地震的波形资料,利用波形拟合法反演了震源机制解及区域应力场.反演结果显示,位于龙门山断裂带上的地震,震源机制以逆冲型为主,鲜水河断裂带地震震源机制以走滑型为主,而川滇块体西南部的理塘断裂、金沙江断裂附近,震源机制解以正断层为主.根据震源机制解反演得到的龙门山地区、鲜水河地区的主压应力场方向为WNW、近EW向.川滇块体的巴塘、理塘等地区,其主压应力轴方向为12°左右,接近SN向,且仰角接近40°左右.本研究利用面波振幅谱特征对震源深度进行了精确定位,定位结果与中国地震台网中心(CENC),美国地震调查局(USGS),国际地震中心(ISC)等机构地震目录进行了对比.结果显示,四川地区强震震源深度主要分布在20km以上的中上地壳.龙门山地区震源优势分布在10～20km,鲜水河断裂地震震源深度在10km左右,川滇块体西南部的理塘断裂,巴塘断裂,金沙江断裂等地区,震源深度一般在5～10km范围. 相似文献
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利用国家测震台网数据备份中心时间跨度超过7年的连续波形资料, 设定至少三个台站记录的垂直分量波形互相关系数大于0.8的地震对为一组重复地震, 通过波形互相关分析, 识别出龙门山断裂带周缘波形相关意义上的“重复地震”2790次, 构成2907组重复地震。 沿用Schaff和Richards的研究结果, 假定“重复地震”间距很小(小于1 km), 地震目录记录的重复地震对位置之差主要为地震台网的定位误差所致, 基于此误差给出了龙门山断裂带周缘地震台网的定位精度估计: 台网的水平定位精度较高, 水平定位误差约为2.8 km(2倍标准差), 且西南段台网的水平定位精度优于中北段; 垂直定位精度较差, 垂直定位误差约为10 km(2倍标准差), 现有地震定位方法对震源深度的测定有待改善。 相似文献
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《地震工程学报》2018,(Z1)
以四川地区2008—2015年期间发生的ML4.0～6.0地震为例,利用四川区域台网宽频带波形资料,采用CAP(Cut and paste)方法计算其震源机制解和最佳震源深度,在此基础上分析地震震源机制解和震源深度空间分布特征。结果表明:(1)四川地区地震震源机制解类型存在显著空间分区特征。逆冲型地震集中分布在龙门山断裂带和川东盆地,揭示青藏高原的巴颜喀拉地块与华南地块的相互作用方式——强挤压。走滑型地震绝大多数分布在川西高原和攀西地区,这是由于印度板块向北东推挤和青藏高原物质向东扩张所导致的上地壳物质沿大型断层滑移。正断型地震主要分布在金沙江断裂带北段和汶川大震主震区,金沙江断裂带北段的拉张应力状态应是由青藏高原东部下地壳物质流动对上地壳物质有拖曳作用,与多力源组合共同作用决定的;而汶川主震区的正断型地震应是主震后震源区不同来源动力作用的复杂应力调整现象。其他类型地震都分布在龙门山断裂带,属于汶川或芦山地震的余震活动,其成因为大震后震源区不同来源应力作用使主应力方向倾斜偏离了水平面和垂直面而引起的应力变形。(2)震源机制解参数中的P、T、N轴反映了地震前后震源区应力状态的变化,是震源区构造应力的一种体现。四川地区构造地震的P、T轴方位空间展布存在地区差异:川西高原地区以约31°纬线为界,北部区域P轴方位呈NEE向,南部区域呈SEE向(平均约E19°S);龙门山断裂带南段P轴方位呈SEE向(平均约E25°S),中、北段P轴方向离散,无优势方位;攀西地区P轴方位呈SE向(平均约E51°S);T轴方位在川西高原呈近SN向拉张,在攀西地区又转为NE向,呈顺时针旋转趋势。(3)四川地区地震震源深度空间分布差异显著。从整体来看,四川地区地壳优势孕震层深度范围为5～15km,深度更深的地震分布在地壳厚度存在异常的大型断裂带(龙门山、小金河断裂带)或盆地至高原的过渡地带(乐山、犍为等地)。龙门山断裂带地震震源深度空间分布呈现出西南深、东北浅的特征,西南段地震震源最深达26km,中、北段地震震源最深达19km;且断裂带上走滑型地震相对于逆冲型和正断型地震存在震源深度偏浅的现象。川东盆地地震震源深度空间分布展显出西南深、东南浅的特征,盆地东南部地震震源深度分布范围为2～5km。揭示出四川地区地震震源是沿活动的脆性上地壳分布。 相似文献
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选取江苏测震台网震中距2°以内18个地震台站记录清晰的波形资料,使用单纯形、LocSAT、HypoSAT地震定位方法,分别采用华南速度模型、郯庐断裂带中南段速度模型以及IASP91全球速度模型,重新测定江苏大丰海域MS5.0地震震源深度,对获取的深度值进行对比分析。结果表明:3种地震定位方法测定的震源深度结果接近,约为11 ± 2 km;HypoSAT定位方法计算结果较为稳定,IASP91、郯庐断裂带中南段模型均适用于该区域震源深度计算。 相似文献
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利用2001年1月至2008年6月四川固定地震台网和临时地震台站记录到的大量P波到时资料,反演了龙门山断裂带及周边地区的地壳精细三维P波速度模型. 结果表明,汶川主震以北和以南地区的结构存在较大差异,以北地区的龙门山断裂带具有很强地壳不均匀性,这与该区发生了大量汶川地震的余震相一致. 这些结果有意义地改进了前人对龙门山断裂带仅为不同块体过渡带的认识. 汶川主震震源区下方存在有明显低波速异常体,表明流体可能存在于龙门山断裂带内. 这些流体可能直接影响汶川大震的形成. 本文的成像结果为下地壳流沿龙门山断裂带上浸提供了可靠的地震学证据. 相似文献
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2013年4月20日发生了四川芦山MS7.0地震,主震中位于青藏地块与华南地块结合部的龙门山断裂带南端.本研究用双差定位法对芦山地震主震及余震序列进行重新定位,得到主震位置为(30.29°N,102.97°E,17.82 km)及4100多次余震重新定位结果.利用GSN/IRIS台网和国家台网及四川省区域台网的波形数据对主震及部分余震进行了震源机制解反演.结果表明,主震为一次逆冲地震,根据余震序列分布确定发震断层面走向为200°,震源机制解断层倾角为45°.基于震源断层面解和断层滑动方向,采用力轴张量计算法得到了研究区域的平均主压应力方向约为N112°E. 相似文献
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宋秀青 《地震地磁观测与研究》2017,38(4):15-20
2017年8月8日四川阿坝州九寨沟县发生M 7.0地震,随后发生一系列余震。该地震发生在川甘交界处四川一侧。国内外科研机构对主震的震源深度给出不同结果。本文采用PTD方法,采用四川省地震台网测定的震相数据,基于四川2015地壳速度模型,计算得到M 7.0主震震源深度为13 km,利用甘肃省地震台网震相数据,基于甘肃2015地壳速度模型,计算得到主震震源深度为12 km。震后流动台架设后,由近台证明PTD测定深度结果的可靠性。另外,计算M 3.0以上余震的震源深度。所有震相数据来自中国地震台网中心编目数据库。 相似文献
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在南北地震带地区,USGS全球地震目录中存在一些震源深度大于30km的地震.这些地震的震源深度是否可靠,对于研究这一地区的孕震机制、岩石圈强度和构造演化等科学问题具有重要意义.本文以南北地震带2012年发生的5个4~5级地震为例,利用区域地震台网的波形数据,基于sPL深度震相、短周期瑞利面波以及CAP等独立方法测定了其震源深度.结果表明:sPL深度震相和CAP方法给出的震源深度比较一致,差别小于2~3km,能够得到比较可靠的震源深度;短周期瑞利面波及其与P波振幅比也确定了地震震源深度较浅的特征.本文研究结果显示:宁夏会宁4.7级、云南富民4.8级和四川会东4.7级地震的震源深度约为8~12km左右,仍为发生于上地壳的地震,USGS地震目录给出的30km甚至更深的震源深度存在明显偏差;对于四川隆昌4.6和4.9级地震,本文给出的震源深度为1~2km,属于极浅源地震,USGS地震目录给出的10km和35km的震源深度结果尚需进一步改进. 相似文献
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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
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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
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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
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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.
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
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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
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