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1.
选取2010—2020年呼和浩特基准地震台记录的195个6.0级以上极远震事件波形,分析震相特征.按照震中距由小到大的顺序,挑选出9个典型极远震事件作为研究对象,依据AK135走时表,分析波形记录特征,以期提高地震台站的震相分析水平及资料产出质量.  相似文献   

2.
震中距100°左右地震震相特征分析   总被引:1,自引:0,他引:1  
震中距100°左右的地震,位于远震与极远震之间,特征既像远震又像极远震,震相较难分析。为了提高对该震中距地震的速报能力,对山西省地震局太原基准地震台记录的该震中距的地震事件进行了分析,总结了其震相特征及规律。  相似文献   

3.
分析了相邻井下、地表地震计记录的背景噪声及近震、远震波形特征,以及相关的振幅谱及近震、远震接收函数波形特征.结果表明,井下地震计记录的背景噪声比地表地震计小1个数量级,其近震、远震波形记录较清晰、简洁;井下、地表地震计记录的远震振幅谱和径向接收函数具有较好的一致性,但背景噪声、近震振幅谱、近震接收函数、远震切向接收函数...  相似文献   

4.
选取乌什、库车台2010~2014年5年内记录到MS5.0~6.8的不同区域较浅中强远震1 648个,对波形与震相统计分析、对比研究,总结特征,再用MATLAB工具对典型震例波形进行转换、滤波等处理,以期清晰提取波形与震相的差异信息,从而更好地推动台站的波形处理与远震分析工作。  相似文献   

5.
以西安地震台记录的2001-2018年13次6级以上极远震为研究对象,依据AK135走时表进行震相分析,总结归纳典型极远震震相记录特征,以期提高震相分析水平和测震分析工作质量,为其他地震台站极远震分析工作提供借鉴。  相似文献   

6.
分析了相邻井下、地表地震计记录的背景噪声及近震、远震波形特征,以及相关的振幅谱及近震、远震接收函数波形特征。结果表明,井下地震计记录的背景噪声比地表地震计小1个数量级,其近震、远震波形记录较清晰、简洁;井下、地表地震计记录的远震振幅谱和径向接收函数具有较好的一致性,但背景噪声、近震振幅谱、近震接收函数、远震切向接收函数波形存在一定差异;由地表地震计得到的近震震级比井下地震计的大0.12,地表地震计到井下地震计之间的P波速度约为2 km/s。  相似文献   

7.
四川汶川系列地震距太原基准地震台约1000km,介于近震与远震之间,震相特殊,识别困难。本文通过对汶川主、余震和四川其他地区远震波形的对照,及对主要震相周期、幅度及波形特点的分析,认为PN、SG两个震相是太原地震台记录四川汶川地震的主要定位震相。  相似文献   

8.
中国东北地区新生代板内火山群广泛发育,其中大兴安岭火山群区的上地幔结构研究匮乏,火山群的演化机理尚不明确.本文收集近年来大兴安岭地区流动台站和固定台站的观测波形数据,通过波形互相关从远震事件记录中挑选出64575个P波震相走时残差,13566个S波震相走时残差,开展远震体波走时层析成像研究,获得该区上地幔的VP、VS以...  相似文献   

9.
BBVS-120型甚宽频带数字地震计典型地震波形记录特征   总被引:1,自引:1,他引:0  
对太原基准地震台BBVS-120型甚宽频带地震计记录的不同震中距及不同类型天然地震和非天然地震波形进行分析和对比,结果表明,该地震计能够清晰记录近震、远震、极远震及爆破、塌陷等震相,对各类地震具有较好的监测能力,基本实现全频带观测,可为获得丰富的震相资料并提升地震台监测能力及速报质量,提供技术保障。  相似文献   

10.
选取乌兰浩特地震台记录到的典型天然地震事件及爆破事件,根据断裂带分布及波形记录特征,分析地震及爆破事件的震相特征。结果表明,研究区域近震波形Pn、Pg、Sn、Sg震相及Sm面波较清晰,Pg、Sg波走时差一般不大于23 s,与中国地震台网中心发布的MS震级间的偏差一般小于0.6级;远震P、S、pP、sP震相可较清晰识别,Pm、L面波记录较明显,P、S波走时差一般不小于25 s,震级偏差一般小于0.4级,且通过震相特征及实地考察发现,爆破多为霍林郭勒区域爆破事件。  相似文献   

11.
In this paper, the data of earthquake events of magnitude MS6.0 and above produced in Hohhot Seismic Station from 2008 to 2015 and the data of ML ≥ 1.0 seismic events from 2015 to 2016 in Horinger Seismic Station and the surrounding mobile stations in southern Hohhot are selected. Using Splitlab and SAM software, the spin-correlation method, the least-energy method and the cross-correlation coefficient method are used to analyze the teleseismic and near-seismic phases (SKS, S). The results of this study are in good agreement with the results previously obtained by other researchers. The study of teleseismic SKS splitting reflects the characteristics of the anisotropy of the upper mantle beneath Hohhot, that is, the anisotropy of the upper mantle shows NW, which reflects "fossil" Anisotropy, mainly in the continental structure of stable units and preserves the history of mantle deformation information. The crustal anisotropy reflected by the near-earthquake S-wave splitting study is similar to that of the active fault zone, trending NE as a whole and is consistent with the tectonic stress field background of the northeastern margin of Ordos block.  相似文献   

12.
刘贤伦 《内陆地震》1994,8(1):43-51
根据1985年4月~1988年10月38次极远震资料,着重分析了乌鲁木齐台不同震中距极远震震相特征,提出了单台分析方法以及分析中应该注意的一些问题,对部分疑难震相进行了分析讨论。  相似文献   

13.
The three-dimension crustal and upper mantle structures in the region around Beijing were studied by seismic tomography. We used the P wave arrival times from local and teleseismic events. These events were recorded by 250 stations of the North China Seismic Array and 108 stations of the Beijing Telemetry Seismic Network. 118 869 P wave arrivals from 10 285 local events and 12 189 P wave arrivals from 107 teleseismic events were used in the inversion. We obtained the 3-D P wave velocity structure of the cru...  相似文献   

14.
Automatic onset phase picking for portable seismic array observation   总被引:1,自引:0,他引:1  
Automatic phase picking is a critical procedure for seismic data processing, especially for a huge amount of seismic data recorded by a large-scale portable seismic array. In this study is presented a new method used for automatic accurate onset phase picking based on the proporty of dense seismic array observations. In our method, the Akaike's information criterion (AIC) for the single channel observation and the least-squares cross-correlation for the multi-channel observation are combined together. The tests by the seismic array observation data after triggering with the short-term average/long-term average (STA/LTA) technique show that the phase picking error is less than 0.3 s for local events by using the single channel AIC algorithm. In terms of multi-channel least-squares cross-correlation technique, the clear teleseismic P onset can be detected reliably. Even for the teleseismic records with high noise level, our algorithm is also able to effectually avoid manual misdetections.  相似文献   

15.
Seismic data recorded at the broad-band teleseismic GRF array and theshort-period regional GERESS array, which is a designated IMS primarystation, are analyzed to determine the effectiveness of teleseismic P-wave complexity for the purpose of seismic event screening within theframework of Comprehensive Nuclear-Test-Ban Treaty verification. For theGRF array, seismic waveform data from nearly 200 nuclear explosions havebeen recorded since its installation in the late 1970's, which were studiedalong with several thousand earthquakes from the last few years.Additionally, we investigated teleseismic P wave complexity for a similarnumber of earthquakes recorded at GERESS. However, owing to itsoperation starting in 1991, only a limited number of nuclear explosionseismograms are available for study.For nuclear explosions, complexity does not exceed levels of 0.3 except fora number of events from the Nevada Test Site recorded only at the GRFarray and located at a large distance where PcP may interfere with the initialP wavelet. Since all events with complexity at GRF larger than 0.3 areexclusively located on Pahute Mesa within the Nevada Test Site,near-source geology or topography must play a dominant role for theseincreased complexity values, while PcP may not contribute significantly tothe high-frequency energy measured by the complexity parameter.Although many earthquakes show complexities below this level, for morethan 25% of the earthquakes investigated the complexities determined arelarger than 0.7, thus showing distinctly larger values than nuclearexplosions. Therefore, this percentage may be screened as earthquakes fromall seismic events detected. As currently only about half of the eventsdetected by the global IMS network are screened out based on focal depthand the m b :M s criterion, teleseismic P-wavecomplexity may contribute significantly to the task of seismic eventscreening.  相似文献   

16.
在北京地震台NCDSN宽频带地震图集编辑工作中,发现Pn波在远至震中距16.8°的地震中仍然作为初至波被清晰记录,而PnPn波则延续至震中距30°左右仍以非常明显的震相特征被记录下来。  相似文献   

17.
选取呼包鄂区域11个宽频带地震台站记录的156个远震事件,使用剪切波分裂软件,对所选远震波形数据进行处理,求取并分析震中距85°—110°范围内同时被各地震台站记录的远震震相SKS的各向异性参数,即快波偏振方向及慢波到时差,结果表明:呼包鄂区域地下深层介质存在各向异性,快波偏振优势方向为ESE,慢波延迟时间为0.87—1.74 s,平均延迟1.26 s,推断该区地下深层介质存在各向异性层,层厚100—200 km,平均层厚约145 km。  相似文献   

18.
三峡地区上地壳结构的远震虚震源反射地震成像   总被引:2,自引:1,他引:1       下载免费PDF全文
远震虚震源反射成像方法利用远震初至波在台网之下地表与地下界面间形成的反射波(PPdp震相)波形资料进行台网地区地震反射结构研究.此方法先用台网各台站的平均初至波形求取震源信号,再用该震源信号与各道地震记录作反褶积从而取得反射剖面.本文介绍了远震虚震源反射成像的基本原理和实现步骤,并以三峡地区的观测资料为例,得到三峡库首区上地壳的反射地震剖面.成像剖面中解释出的四川盆地和秭归盆地的底界面位置和形态与地表地质观测和大地构造背景吻合.为验证虚震源成像的能力,本文使用弹性波正演模拟合成地震数据,经过处理实际资料一样的步骤获得虚震源成像结果.正演模拟表明,叠加多个远震的反射地震剖面可以有效地改善成像的信噪比和连续性;虚震源成像需要选择特定的震源频率范围,以减轻高频噪音以及低频造成的成像问题.在研究上地壳结构时,建议在不适合主动源采集和缺乏低频信号的地区尝试远震虚震源方法.  相似文献   

19.
海拉尔CTBTO地震台阵下方小尺度非均匀体研究   总被引:1,自引:0,他引:1       下载免费PDF全文
利用国际禁核组织在海拉尔布设的小孔径地震台阵的16个深远地震波资料,分离出了P波波场中不相干的尾波.频率域中对波场扰动的研究表明,在0.5~3.0 Hz的频率范围内,观测到的波场扰动可以利用P波在随机介质中的散射进行解释.不同远震事件得到的稳定结果表明,在该台阵下方34 km厚的地壳和110 km厚的岩石层中可能存在相关长度为2.0~7.4 km的散射体.  相似文献   

20.
In recent years, the measurement of rotational components of earthquake-induced ground motion became a reality due to high-resolution ring laser gyroscopes. As a consequence of the fact that they exploit the Sagnac effect, these devices are entirely insensitive to translational motion and are able to measure the rotation rate with high linearity and accuracy over a wide frequency band. During the last decade, a substantial number of earthquakes were recorded by the large ring lasers located in Germany, New Zealand, and USA, and the subsequent data analysis demonstrated reliability and consistency of the results with respect to theoretical models. However, most of the observations recorded teleseismic events in the far-field. The substantial mass and the size of these active interferometers make their near-field application difficult. Therefore, the passive counterparts of ring lasers, the fiber optic gyros can be used for seismic applications where the mobility is more important than extreme precision. These sensors provide reasonable accuracy and are small in size, which makes them perfect candidates for strong motion applications. The other advantage of fiber optic gyroscopes is that if the earthquake is local and shallow (like one occurred early this year at Canterbury, New Zealand), the large ring lasers simply do not have the dynamic range??the effect is far too large for these instruments. In this paper, we analyze a typical commercially available tactical grade fiber optic gyroscope (VG-951) with respect to the seismic rotation measurement requirements. The initial test results including translation and upper bounds of seismic rotation sensitivity are presented. The advantages and limitations of tactical grade fiber optic gyroscope as seismic rotation sensor are discussed.  相似文献   

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