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1.
尽管Pn波品质因子(PnQ)对上地幔流变性质研究及核试验监测有着深刻含义,迄今它仍然是一个难以准确测定的地震参量.这是因为除了众所周知的影响所有短周期Q的干扰因素外,在所有主要的区域震相中,地震工作者对Pn波的传播模式及几何扩散函数G=d-k中的扩散率指数k了解最少.不同的研究者任意地假定不同的常数k,因此常算出非常不同的PnQ值(例如文献[1]、[2]).实际上,理论研究已表明,k随频率而变,变化的形式取决于上地幔的速度结构.本文介绍用一推广的逆向双台法同时测定加拿大东部的PnQ和k值.我们的结果表明:1.加拿大东部的Pn波是由一系列的干涉潜波叠加而形成;2.视PnQ(散射和固有非弹性的综合效应)随频率而增加,在15Hz处接近2000.  相似文献   

2.
射线追踪法是一种有效的地震波场数值模拟方法,在层析成像、叠前深度偏移及正演模拟等研究领域均占据重要地位.但相较于波动方程数值模拟方法,射线追踪法在获取较高运算速度的同时损失掉了地震波场的动力学信息,对于整个地震波场的地震波衰减以及转换波等问题都没有进行考虑.为了能够得到较为完整的合成地震记录并对地震资料做出更合理解释,本文在使用射线追踪法进行波场数值模拟的同时考虑了衰减信息,追踪转换波以弥补射线追踪法在动力学上的缺陷.在全波射线追踪过程中,通过追踪同类波和转换波,并计算该段射线的能量衰减,在保证高速计算的同时获得了较为完整的合成地震记录,取得较好的效果.  相似文献   

3.
槽波地震勘探利用槽波的频散特性反演煤层的结构特征,故理论频散曲线的计算是一个重要方面.使用水平层状模型假设下的面波频散曲线计算方法能够计算煤层厚度恒定模型地震槽波频散曲线;但当煤层厚度变化时该方法不再适用.基于前人水平层状均匀介质模型的面波理论频散曲线计算方法,对于含煤三层模型,本文发展了煤层厚度变化情况下的地震槽波理论频散曲线计算方法,并使用该方法计算分析了不同厚度函数模型的频散曲线形态特征.研究表明:与稳定厚度煤层相比,煤层厚度变化使得地震槽波群速度成为与频率及传播射线在水平面投影路径相关的二元函数;射线路径上煤层厚度的变化使得频散曲线在群速度方向上压缩,群速度变化范围变小,且使处于最小值位置的埃里相群速度增大;而煤层厚度的线性变化模型频散曲线只与射线首、尾处的煤层厚度有关,与煤层厚度恒定模型相比,曲线形态不发生改变;煤层厚度呈非线性变化时,频散曲线形态上可能发生改变.  相似文献   

4.
利用重复地震研究滦县地区的地壳介质变化   总被引:1,自引:1,他引:0  
运用双差定位法,对滦县地区2002年1月至2010年8月ML≥2.0地震进行精定位,利用射线追踪方法,对滦县地区的重复地震进行位置归一处理,计算滦县地区重复地震序列经过射线追踪方法校正后得到的P波走时差变化.研究发现,2010年3月6日滦县ML4.7地震前糙甸地震台、兴隆东地震台、蓟县地震台和遵化地震台记录到P波走时差...  相似文献   

5.
波路径偏移压制层间多次波的理论与应用   总被引:4,自引:4,他引:0       下载免费PDF全文
消除层间多次波是地震勘探资料处理研究领域的难题,尤其对于实际资料的处理,到目前为止还很难找到一种完全有效的方法. 本文给出了仅对一次波成像既波路径偏移方法压制层间多次波方法,在共炮道集和共检波点道集分别计算炮点射线的入射角和检波点射线的出射角,由此计算的角度作为射线追踪的初始角度,计算地震波射线的传播路径. 结合由程函方程计算的走时表,判断偏移范围是反射波还是多次波. 在前期偏移过程压制多次波的理论研究基础上,本文主要研究波路径偏移消除多次波的应用部分. 为了进一步说明效果的有效性,计算了在单炮和共成像点道集压制层间多次波,给出了实际资料的压制多次波的偏移结果.  相似文献   

6.
运用双差定位法对滦县地区2002年1月至2010年8月ML≥2.0级地震进行精定位,利用射线追踪方法对滦县地区的重复地震进行位置归一处理,计算了滦县地区重复地震序列经过射线追踪方法校正后得到的P波走时差变化.研究发现,2004年1月20日滦县ML5.0级和2010年3月6日滦县ML4.7级2次中等地震前所选取的测震台站...  相似文献   

7.
选取2010年1月至2022年4月重庆地震台网记录的荣昌地区92次ML≥2.5地震观测资料,采用射线追踪方法,对荣昌地区重复地震震源位置做归一化处理,分别计算4个方位上所选台站记录的地震P波走时差,结果显示:研究区域NE、SE和SW方位台站记录的地震P波走时差负异常持续时间较长(其绝对值较大),表明地壳介质波速有明显升高现象。  相似文献   

8.
福州-泉州-汕头地区地壳结构的爆炸地震研究   总被引:71,自引:7,他引:71       下载免费PDF全文
本文根据1982和1985年在福州-泉州-汕头地区的人工爆炸地震测深资料,分析了震相特征,共识别到九个波组:P1、Pg、Pg、P3°、P4(P4°)、P5°、Pn(Pn°)、P7*及S波组。通过对波的走时反演、正演拟合、理论地震图和射线追踪方法反复计算,得到了该区地壳与上地幔结构模型。结果表明,该区具有大陆地壳向海洋地壳过渡的边缘地区结构特征。地壳P波速度6.30km/s,莫霍面速度7.90km/s,地壳厚度30km,由三层构成,厚度分别为3km、15km和12km。在中地壳存在一层速度为5.50-5.90km/s、厚度为3.0-4.0km的低速层,低速层分布与温泉出露有密切的关系。在下地壳下部有一数公里厚的高速致密的壳-幔混合物层,其形成原因是由于上地幔物质上涌并迁移到下地壳的结果。此外,还讨论了莫霍面结构,界面起伏和断裂展布概况。  相似文献   

9.
利用重复地震研究广东阳江地区地壳介质变化   总被引:4,自引:0,他引:4  
叶秀薇  闻则刚  刘锦  杨马陵  胡秀敏 《地震》2008,28(4):103-111
利用射线追踪方法对广东阳江地区的重复地震进行位置归一处理, 提高走时精度以达到观测地壳介质变化的目的。 文中计算了阳江地区2002年1月至2007年9月ML≥2.0重复地震序列经射线追踪法校正后的P波走时差。 结果显示, 在2004年阳江4.9级地震前信宜台、 湛江台、 肇庆台的记录观察到该地区短期的地壳介质速度明显升高的现象。  相似文献   

10.
2014年8月3日云南鲁甸发生M_S6.5地震,造成重大人员伤亡和财产损失。此次地震发震构造复杂,引起了地震学界的广泛关注。本文基于三维建模方法,建立鲁甸地区三维层状非均匀速度模型,采用逐段迭代射线追踪方法对鲁甸M_S6.5地震进行三维射线追踪走时计算;利用震中距150km范围内的近震Pg波震相走时数据,通过射线追踪走时拟合获得鲁甸地震的震源深度约为12km,与前人研究成果基本一致,表明了本文采用的三维建模和射线追踪方法的有效性。  相似文献   

11.
本文介绍了宇宙线空间物理学在我国的形成和主要研究内容,包括:(1)空间探测,有火箭探测、卫星探测;地面宇宙线台站观测;宇宙线的水下测量;(2)宇宙线空间物理学研究,有宇宙线的日地传输;宇宙线强度变化与CME事件;宇宙线的源物质与加速过程;宇宙线的地球物理效应.最后提到宇宙线与人体健康,特别是流行性感冒、大的太阳质子事件与地震现象、太阳宇宙线事件与天气和气候等的统计研究.  相似文献   

12.
用两种数据处理方法对2008年5月12日14时28分发生的8.0级汶川大地震前和地震发生时北京、广州、Moscow、Irkutsk和Nagoya五个台站的宇宙线变化幅度特性进行了分析.研究发现,地震前、地震时北京台站的宇宙线强度均有一定的响应,其变化幅度分别达到了1.15%, 1.31%,而其它台站没有明显的响应,这可能为我们以后利用宇宙线对大地震进行警报提供了研究基础.  相似文献   

13.
复杂速度模型的地震交切定位方法   总被引:3,自引:0,他引:3  
交切法是最基本的地震定位方法之一,该定位方法具有稳定性强、速度快的优点。由于速度模型假设为均匀或水平均匀介质,与实际介质有较大偏差,因此定位精度较低,特别是震源深度。为克服传统交切法的缺点,我们对其进行了改进。在改进的方法中,震源轨迹不再假设为圆形或双曲线形,而是利用最小走时树射线追踪方法进行精确计算。数值模型计算表明,本文提出的改进方法,可用于复杂速度模型的地震定位。  相似文献   

14.
Traveltime computation by wavefront-orientated ray tracing   总被引:1,自引:0,他引:1  
For multivalued traveltime computation on dense grids, we propose a wavefront‐orientated ray‐tracing (WRT) technique. At the source, we start with a few rays which are propagated stepwise through a smooth two‐dimensional (2D) velocity model. The ray field is examined at wavefronts and a new ray might be inserted between two adjacent rays if one of the following criteria is satisfied: (1) the distance between the two rays is larger than a predefined threshold; (2) the difference in wavefront curvature between the rays is larger than a predefined threshold; (3) the adjacent rays intersect. The last two criteria may lead to oversampling by rays in caustic regions. To avoid this oversampling, we do not insert a ray if the distance between adjacent rays is smaller than a predefined threshold. We insert the new ray by tracing it from the source. This approach leads to an improved accuracy compared with the insertion of a new ray by interpolation, which is the method usually applied in wavefront construction. The traveltimes computed along the rays are used for the estimation of traveltimes on a rectangular grid. This estimation is carried out within a region bounded by adjacent wavefronts and rays. As for the insertion criterion, we consider the wavefront curvature and extrapolate the traveltimes, up to the second order, from the intersection points between rays and wavefronts to a gridpoint. The extrapolated values are weighted with respect to the distances to wavefronts and rays. Because dynamic ray tracing is not applied, we approximate the wavefront curvature at a given point using the slowness vector at this point and an adjacent point on the same wavefront. The efficiency of the WRT technique is strongly dependent on the input parameters which control the wavefront and ray densities. On the basis of traveltimes computed in a smoothed Marmousi model, we analyse these dependences and suggest some rules for a correct choice of input parameters. With suitable input parameters, the WRT technique allows an accurate traveltime computation using a small number of rays and wavefronts.  相似文献   

15.
The purpose of this paper is to discuss the statistical distributions of recurrence times of earthquakes. Recurrence times are the time intervals between successive earthquakes at a specified location on a specified fault. Although a number of statistical distributions have been proposed for recurrence times, we argue in favor of the Weibull distribution. The Weibull distribution is the only distribution that has a scale-invariant hazard function. We consider three sets of characteristic earthquakes on the San Andreas fault: (1) The Parkfield earthquakes, (2) the sequence of earthquakes identified by paleoseismic studies at the Wrightwood site, and (3) an example of a sequence of micro-repeating earthquakes at a site near San Juan Bautista. In each case we make a comparison with the applicable Weibull distribution. The number of earthquakes in each of these sequences is too small to make definitive conclusions. To overcome this difficulty we consider a sequence of earthquakes obtained from a one million year “Virtual California” simulation of San Andreas earthquakes. Very good agreement with a Weibull distribution is found. We also obtain recurrence statistics for two other model studies. The first is a modified forest-fire model and the second is a slider-block model. In both cases good agreements with Weibull distributions are obtained. Our conclusion is that the Weibull distribution is the preferred distribution for estimating the risk of future earthquakes on the San Andreas fault and elsewhere.  相似文献   

16.
By analyzing seismograms of short period records at the Beijing SeismoJogicaJ Observatory, the present paper investigates the amplitude ratio of seismic phases. The results indicate that the amplitude ratio of Sn/Lg is correlated with the lithosphere structure, the thermal state, and strong earthquake occurrence in the region the seismic rays pass through. The significance of such a correlation in the study on the genesis and prediction of strong earthquakes is discussed.  相似文献   

17.
Double-difference tomographic methods use directly accurate time delays computed between similar signals. Such methods are designed to image very heterogeneous media, such as volcanoes or fault zones. In seismological applications, similar signals are recorded at a given station from earthquakes sharing similar and close-by sources. In seismic exploration experiments, similar signals are often recorded at neighbouring receivers. After a brief presentation of the tomographic algorithm used, a seismological application is summarized. The potential and limits of double-difference tomographic methods are explored using various numerical experiments. They show that two effects are competing in double-difference tomography: (i) the degradation of the stability of the inversion due to the geometrical proximity of the rays used in the differentiation and (ii) the decrease in modelling error, which allows improving the stability of the inversion and using smaller quantities of a priori information when data are sufficiently accurate. The best resolution is obtained for an optimal value of the inter-source or inter-receiver distance. For optimal values of these distances and a priori information, tomography using traveltime differences provides significantly better resolved results than using traveltimes.  相似文献   

18.
相继发生的三个强震的分布关系   总被引:5,自引:0,他引:5  
邓志辉  马瑾 《地震地质》1991,13(2):173-178
本文从动态的观点出发,把时间上相继发生的三个7级以上强震(设它们分别为A、B和C事件)在空间上的分布关系作为主要研究内容。研究结果表明:(1)ABC所在平面的优势分布是切过软流圈的顶部或岩石圈的下部;(2)在地震A和B发生之后,地震C的优势分布是位于A,B连线的延伸部分和A,B之间稍近A的部位。根据A,B,C的分布关系,结合各地区的地质条件和历史地震资料等,我们可以从已知的两个7级以上强震预测第三个7级以上强震在各地区的发震概率大小  相似文献   

19.
我国近海地震活动特征及其与地球物理场的关系   总被引:1,自引:1,他引:0       下载免费PDF全文
对我国近海海域有历史记载以来的地震的震级、震中参数进行了整理分析,并分析了各海域地震活动的时、空分布规律,根据历史地震资料,确定海域受历史地震影响的最大影响烈度,然后初步分析了地震活动与现代构造应力场、地球物理场的关系.研究发现:(1)近海海域历史地震资料的精度较低,中强地震存在明显的遗漏.(2)渤海、台湾海峡、南海北部地震活动性较强,黄海次之,东海最弱.(3)近海海域的震害主要来自海域地震和近岸陆地强震的影响,影响强弱依次为:渤海、黄海、东南沿海、东海.(4)现代构造应力场以水平向构造应力场作用下的走滑运动为主,最大主应力方向受印度板决和太平洋板块、菲律宾海板块的俯冲挤压方向影响.(5)海域地球物理场,特别是布格重力异常、地壳厚度分布与强震构造带的空间分布关系的相关性较好.本文的研究结果可为我国海域及滨海重要工程的抗震设防、海域地震危险性区划提供一定的基础.  相似文献   

20.
The attenuation characteristics and site response are calculated respectively for each individual tectonic unit in Sichuan (Sichuan Basin,west Sichuan plateau and Panzhihua-Xichang area),using digital waveform data recorded by regional seismic networks and relevant seismic phase data collected from China Seismograph Network.The frequency dependent Q(f) is obtained by the iterative grid-search technique described by Atkinson and Mereu based on trilinear geometrical spreading model.The source spectra are determined by the model of Brune and the site responses of seismic stations are derived by Moya's method using genetic algorithms.Comparison to conventional ML estimates shows that the network local magnitude bias is quite significant at low and intermediate magnitudes.The bias at the jth station for the ith event is defined as ΔMij=Mij-Mi, where ΔMij is the station magnitude and Mi the network-average value.For comparison,we mapped the spatial distribution of biases by digital seismograms recorded from 10535 earthquakes of magnitude 2.5≤ML≤4.9 that occurred in Sichuan from January 1,2009 to June 30,2015.Based on the above data,the attenuation characteristics,site response and their effects on magnitude determination in Sichuan are analyzed.Our results demonstrate that the associated model for regional quality factor for frequencies can be expressed as Q1(f)=450.6f0.513 4 for Sichuan Basin,Q2(f)=136.6f0.581 3 for west Sichuan Plateau and Q3(f)=101.9f0.666 3 for Panzhihua-Xichang area.Site response results indicate that different stations show different amplifications.Maps of biases appear to be different,but with similar dominant spatial distribution.For stations in Sichuan Basin,their greater magnitudes are functions of low attenuation in structure and amplification effects of both seismic stations and basin effects.For stations in west Sichuan Plateau,the possible causes of these lower magnitudes are severe dependence upon source region due to extreme lateral variations in either structure or path effect attenuation.For stations in Panzhihua-Xichang area,broken medium caused by strong tectonic activity or large earthquakes and heat flow up-welling along active faults may be the main reasons of low magnitude values when earthquakes occur in western Sichuan and eastern Tibetan region.And the greater magnitudes for earthquakes along the Longmen Mountains appear to be well correlated with edge effect of sedimentary basin on strong ground motion.In our study,stations magnitude biases appear to be extremely correlated with tectonic structures and different regions when seismic rays passing through,magnitudes are affected significantly by lateral variations in attenuation characters rather than site responses.  相似文献   

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