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1.
针对测震台网台站方位角普查校正实际需要和方位角普查工作技术要求,提出测震台网台站方位标志安装、台站新安装地震计方位测定、已运行台站地震计方位角普查校正的操作方法,以及摆墩与摆坑型场地地震仪输出极性的检测判定方法。  相似文献   

2.
针对测震台网台站方位角普查校正实际需要和方位角普查工作技术要求,提出测震台网台站方位标志安装、台站新安装地震计方位测定、已运行台站地震计方位角普查校正的操作方法,以及摆墩与摆坑型场地地震仪输出极性的检测判定方法。  相似文献   

3.
选取2019—2020年西藏、云南、四川、青海、新疆地震台网记录的MS≥5.5远震事件P波数据,采用P波质点运动方法,计算中国西北、西南地区211个地震台站方位角及其随时间的变化。结果显示,约53%的台站方位角偏差绝对值始终小于3°,运维状况极佳;约39%的台站方位角偏差绝对值保持在3°—10°,运维良好;约9%的台站方位角偏差绝对值大于10°,少数台站存在极性反转等现象。在运行维护过程中,部分台站受到更换或移动地震计等人为因素的影响,地震计方位角出现短时跳变现象。为保证地震数据的可靠性,应定期对台站方位角进行检查和校正,以便为地震学研究提供可靠的基础数据。  相似文献   

4.
南通地震台该旋观测值从2001-08起大幅下降,经过与其他台站资料的比较和仪器工作情况的分析,认为异常不是地磁本身的异常变化,也不是仪器的问题。进一步对外界环境调查和实地测试,证实是受台站附近基建工地的干扰影响。  相似文献   

5.
通过新疆强震台站的加速度传感器极性检测和方位角校正工作,发现新疆强震台站加速度传感器方位角最大误差为83.7°。按照国家强震动台网中心强震台站加速度传感器安装规范,加速度传感器方位角误差应该严格控制在2°以内,经过校正后,新疆区内全部强震台站的加速度传感器方位角误差都控制在1°以内,在很大程度上提高了新疆强震动台网的数据质量和可靠性。  相似文献   

6.
首先采用P波、 SV波和SH波的极性和振幅比联合求解2014年安徽省金寨ML3.9震群序列的震源机制解, 并在此基础上计算得到该震群序列的震源一致性参数和P轴方位角随时间的变化; 然后基于震区附近3个台站记录到的该震群序列的地震波形, 计算其体波谱振幅相关系数, 同时读取震区附近3个台站记录到的该震群序列中115次ML≥1.5地震的极性. 研究结果表明: 金寨ML3.9震群序列的地震震源机制解绝大多数为压性走滑型, P轴方位角较为一致; 其震源一致性参数处于较低水平, 体波谱振幅相关系数较高; 台站所记录到的地震极性也较为一致. 该结果表明金寨ML3.9震群序列的震源一致性程度非常高.   相似文献   

7.
现代地震研究依赖于可靠的三分量观测数据,地震计的北分量是否严格指北将直接影响研究的准确性。然而,受台站附近磁异常或人为安装错误的影响,地震计的方位角可能出现偏差。基于东北地区154个固定台站2020年的远震数据,利用P波质点运动方法,估算了每个台站的北向分量方位角,以判断台站地震计是否存在方位角偏转问题。结果表明,84%的台站运行良好,12%的台站存在方位角偏差绝对值过大(>20°)或分量极性反转等问题。此外,分析后发现方位角偏转较大会导致H-κ叠加方法计算得到的地壳厚度和地震波速比出现偏差。因此,为确保地震学分析的可靠性,固定台站的地震计方位角需要进行定期校标。  相似文献   

8.
天然地震和爆破事件识别是地震监测预警的重要内容.近年来,快速发展的深度学习算法以其强大的数据特征挖掘和图像识别能力,能够较快并准确地约束地震事件属性.利用多输入卷积神经网络算法构建天然地震和爆破事件自动分类网络模型,其中输入信息包括多台站地震波形和单台站的地震时频数据,使得卷积神经网络同时获取事件的波形、频谱和极性特征...  相似文献   

9.
严川  许力生 《地球物理学报》2014,57(8):2555-2572
基于数十年来已有的研究进展,提出了一种地方和区域地震震源机制反演技术——广义极性振幅技术(GPAT),并通过一系列数值实验检验了这种技术的可行性和抗干扰能力.首先,从地震波场概念出发,利用P波初动极性与广义震相振幅构建矢量,建立反演系统,并给出求解技术;然后,考虑影响反演结果的各种因素,包括台站布局、台站数目、随机噪声、震中位置误差、震源深度误差和速度模型误差,分别进行了单一因素影响测试;最后,同时考虑各种因素进行了综合测试.实验结果表明,GPAT是可行的,具有良好的抗干扰能力.需要强调的是,在众多影响因素中,速度模型误差对反演结果的影响最大.  相似文献   

10.
引言 在“九五”项目的实施中,我国地磁观测台站已基本上配备了数字化记录的磁通门磁力仪和分量质子旋进磁力仪。高精度的CTM-DI仪磁通门经纬仪和G856质子磁力仪等绝对观测仪器也得到了普遍应用。有些台站仪器配置甚至更高,进口相对记录仪和绝对观测仪同国产仪器并行运行。但是,地磁观测任务决定了台站不能在架设数字化仪器的同时,立即停止原有模拟记录仪器,也就是说,各套仪器必须有一个并行运行期,这样做有利于数据对比分析及观测数据的连续可靠,进而分析仪器本身的性能,进一步做好数字化改造工作。在地磁台站,数字化改造改变…  相似文献   

11.
This paper describes an adaptation of the ‘leap-frog’ method of barometric altimetry which enables altimetric surveys to be undertaken by a single operator using a single barometer with no requirement for base stations. The method involves two readings at each station, the first bracketed by readings at the previous station, and the second bracketed by readings at the subsequent station. Linear interpolation is used to estimate what the readings would have been at each station at the time that readings were taken at the adjacent stations. Under suitable meteorological conditions errors are generally less than ±1 m, which is sufficiently accurate for a wide variety of geomorphological applications. The method has significant advantages in terms of cost and/or time over more accurate methods such as electronic distance measurement surveys or survey quality global positioning systems. The paper is accompanied by a Microsoft Excel template spreadsheet, BAROSURV.XLT, which converts temperature and pressure readings to relative elevations, and graphs the results. Notes on the use of BAROSURV.XLT are included in the ASCII text file BAROSURV.NOT.  相似文献   

12.
On 22 January 2003, the M w?=?7.6 Tecomán earthquake struck offshore of the state of Colima, Mexico, near the diffuse triple junction between the Cocos, Rivera, and North American plates. Three-hundred and fifty aftershocks of the Tecomán earthquake with magnitudes between 2.6 and 5.8, each recorded by at least 7 stations, are relocated using the double difference method. Initial locations are determined using P and S readings from the Red Sismológica Telemétrica del Estado de Colima (RESCO) and a 1-D velocity model. Because only eight RESCO stations were operating immediately following the Tecomán earthquake, uncertainties in the initial locations and depths are fairly large, with average uncertainties of 8.0?km in depth and 1.4?km in the north?Csouth and east?Cwest directions. Events occurring between 24 January and 31 January were located using not only RESCO phase readings but also additional P and S readings from 11 temporary stations. Average uncertainties decrease to 0.8?km in depth, 0.3?km in the east?Cwest direction, and 0.7?km in the north?Csouth direction for events occurring while the temporary stations were deployed. While some preliminary studies of the early aftershocks suggested that they were dominated by shallow events above the plate interface, our results place the majority of aftershocks along the plate interface, for a slab dipping between approximately 20° and 30°. This is consistent with the slab positions inferred from geodetic studies. We do see some upper plate aftershocks that may correspond to forearc fault zones, and faults inland in the upper plate, particularly among events occurring more than 3?months after the mainshock.  相似文献   

13.
求震源机制P波初动解的格点尝试概率法   总被引:9,自引:0,他引:9  
考虑到P波初动数据在震源球面上分布的不均匀性对节面解的可能影响,不用矛盾符号所占比例的大小作为选择可取节面解的标准,而是将震源球面分成许多小块,再确定有P波初动数字的小块为正号区或负号区的概率,最后以全部有数据小块的平均概率的高低作为选择解答的标准。用此改进方法重新测定了徐纪仁等(Xu et.al,,1988)发表的青藏高原地区99个地震的震源机制解,从中筛选出了20个可信的解答。  相似文献   

14.
Selected problems related to accurate hypocenter locations are discussed in the difficult case that only reliable P-wave readings are available. Near stations are usually only few, and often have a poor azimuthal coverage. As such, they are insufficient because the inversion is highly ill-posed, and the epicenter position strongly trades-off with depth. Thus more distant stations are also needed to obtain the correct epicenter. However, joint use of near and distant stations present another difficulty; it may yield a significantly incorrect depth estimate in case that the crustal model is not fully appropriate. In practice, the erroneous depth often remains unrecognized. An indication of the depth problem can be obtained by analyzing the travel-time residuals at individual stations. It is also useful to check fully independent depth estimates, for example those from the centroid-moment-tensor analysis. If the problematic crustal model is detected, and it is not easy to find a better one, the near- and distant station effects should be decoupled (a two-step location): the epicenter is calculated from all stations, kept fixed, and the source depth is grid-search beneath the epicenter by means of the near stations. The ideas are applied to the Mw 5.2 Efpalio (Western Greece) earthquake of January 18, 2010, and the following aftershock sequence.  相似文献   

15.
1936年4月1日广西灵山县东北M6 ?地震震源参数测定   总被引:1,自引:1,他引:0       下载免费PDF全文
本文收集了1936年4月1日2时至3时(UTC)全球168个台站的仪器记录, 根据1936年4月1日广西灵山县东北部M6 ?地震的宏观震中(22.5°N,109.4°E)和计算所得各台站初至P波的到时残差,将168个台站的数据与灵山主震进行关联或相关性分析.最终有13个台站的数据与灵山主震关联成功,其中7—8个台站的到时数据参与了定位计算.分别利用我国国家测震台网的常规定位方法和技术以及ISC的定位方法和技术对灵山主震进行重新定位,两种重定位方法得到的灵山主震震中相距47.6 km,经过比较,我国国家测震台网的定位方法和技术更适合灵山主震的数据特点.   相似文献   

16.
The analysis of the records from IRIS broadband seismic stations revealed wave trains with a period of ~129.5 min emerging after the strong earthquakes. These wave trains are simultaneously observed at the stations shifted by 180° in longitude in the form of the oscillations with opposite polarity. The occurrence time of the wave trains at the different stations testify to their westward migration by 2.5° per hour. The wave trains are earlier recorded at the stations that are close to the earthquake’s epicenter and to its antipode; they become less manifest with the increase in the distance from the station to the line connecting the epicenter with its antipode. The amplitude of the oscillations in the wave trains is estimated at a few mm and μGal. The wave trains presumably reflect the emergence of an area of free postseismic flexural oscillations of the lithosphere.  相似文献   

17.
This paper describes a new method for reconstructing the polarity of the interplanetary magnetic field. The technique is based on the Svalgaard-Mansurov effect. We ause geomagnetic data of high-latitude stations with a long observation period, including the presatellite era. This method is designed to improve the quality and accuracy of reconstructed polarity, complementing the results of previous methods of Svalgaard (1975) and Vennerstr?m et al. (2001). For the large presatellite period from 1926, the accuracy of the method is estimated to be around 89% of overlaps with the interplanetary magnetic field polarity determined from satellite data.  相似文献   

18.
本文用最大相关时间描写两台地磁场垂直分量日变形态的位相关系。通过恰当的数据处理方式,从两台(北京台和武汉台)地磁垂直分量的整点值计算出最大相关时间。它的平均值等于两台的地方时差。此外最大相关时间还有明显的以年为周期的季节性变化,变化幅度约为0.7小时。对最大相关时间作了傅氏分析,结果表明它含有周期为29.8±0.6天和13.7±0.2天,振幅约为0.06小时的周期变化。  相似文献   

19.
由大量的地震资料推断的我国大陆构造应力场   总被引:77,自引:22,他引:77  
利用多个小地震的P波初动方向数据推断了新疆和西藏部分地区主应力轴的方向.根据以前华北、东部大陆和西南地区的工作结果,对个别地区补充新数据后重新作了分析;加上本文关于新疆和西藏地区的新结果,编制了我国大陆的地震构造应力场方向图.利用Brillinger等的概率模型,估计了用多个地震P波初动方向推断平均P、T轴的误差.讨论了单个大地震震源机制解的P轴与所在地区平均P轴方位角的差异.总结了我国大陆地震构造应力场的主要特征.  相似文献   

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