首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 140 毫秒
1.
用Moya方法反演云南数字地震台站场地响应   总被引:7,自引:2,他引:5  
采用云南区域数字地震台网记录到的178个M≥3.0地震的S波资料,运用Moya方法反演了其中22个子台的场地响应。结果表明,在1~15Hz范围内,22个子台的场地响应都与频率相关,其中3个台的场地响应接近1、平稳变化;11个台站低频部分场地响应接近1、高频衰减;7个台站低频部分场地放大、高频衰减,1个台站场地放大明显。  相似文献   

2.
准确的衰减特征及台站响应对于定量确定地震台网观测环境和分析其构造机制具有重要意义。选取2008—2017年辽宁数字地震台网地震波形资料,利用Lg波谱比与台站场地响应联合反演方法,获得了1~7 Hz Lg波三分向(UD,NS,EW)衰减关系,参与评估的32个台站的场地响应幅值曲线较为平滑,各频段衰减效应存在差异。大多数台站的场地效应幅值在1~8,少数台在低频或高频段上呈现放大效应,最大的幅值近16。结果表明:辽宁地区为低Q0(对应频率1 Hz)和低频率依赖性的构造活跃区,场地响应特征与浅层结构及地质构造有密切关系。不同场地类型的场地响应特征差异明显:井下场地类型的场地响应在低频段内(1~2 Hz)有明显的放大效应;地表较山洞场地类型的场地响应幅值在径向和垂向上都有抬升;相同场地类型中,场地响应放大效应在径向上比垂向上大的多,可能与台基岩性特征有关,而岩性差异对场地响应特征的影响不明显。  相似文献   

3.
基于2016年1月21日青海门源6.4级地震100个MS≥1.0余震序列资料,运用Atkinson法测得青海门源地区Q值,并用Moya法反演了其中24个台站的场地响应。结果表明:在1~20 Hz范围内24个子台的场地响应与频率有关,其中位于震中南部的11个台站场地响应平稳变化,接近1;位于震中东南的11个台站场地响应在低频部分接近1,高频部分衰减至0.1;震中西南的2个台站场地响应高频部分持续放大后衰减。  相似文献   

4.
利用2016年云南测震台网记录到的地脉动数据,运用H/V谱比法计算分析了47个测震台站在0.1~20.0Hz频段内的场地响应。选取2012~2016年期间云南测震台网记录到的ML≥2.5地震做单台震级偏差统计分析,挑出受场地放大作用而出现单台震级大于台网平均震级的台站做去场地放大校正,然后重新统计单台震级偏差情况。计算结果显示云南测震台网的台站受台基条件和所处位置等地质构造因素影响,均存在一定程度的场地放大作用,大部分台站场地响应的卓越频率为1~6Hz,放大倍数为2~4倍。受场地放大作用的影响,大姚、芒市等19个台站的单台ML震级大于台网平均震级。在去除场地放大作用后,台站单台震级与台网平均震级的偏差有所减小。  相似文献   

5.
利用2010年以来河北省测震台网记录到的654个M_L≥2.5地震波形数据,使用Moya方法联合反演计算震源谱及各台站场地响应。河北省测震台网实时接收168个台站数据,最终反演得到151个测震台站场地响应结果。结果显示,频率1~20Hz内各台站均存在不同程度的场地放大效应,随着频率的变化,各类基岩台的场地响应变化较为复杂。位于第四系沉积类的台站场地响应在低频段1~8Hz内放大效应显著,在高频段8~20Hz内呈现快速衰减趋势。选取2017年以来河北省测震台网记录的M_L≥2.0地震数据,对各台站单台震级与台网平均震级进行对比统计、分析,最终得出代表河北地区的地方性震级M_L新量规函数。针对2020年7月12日河北唐山5.1级地震,利用本文得到的台站场地响应结果对震级偏大且有放大作用的台站进行放大作用消除,再分别用现用地方性震级M_L量规函数和河北地区地方性震级M_L新量规函数对单台震级进行重新计算,结果显示震级偏差均有所减小。  相似文献   

6.
用Lg波资料反演场地效应与地震波衰减参数   总被引:4,自引:1,他引:3       下载免费PDF全文
朱新运  陈运泰 《地震学报》2007,29(6):569-580
基于谱比法,以台站记录地震波频谱为观测数据,通过扣除仪器响应及几何扩散后同一地震不同台站记录谱比,扣除震源方向性、 震源因子的影响,在此基础上,建立数学模型通过联合反演求解场地效应及地震波衰减参数. 以浙江省地震台网台站记录的台湾地震数字化地震波资料为基础,使用地震波记录中的Lg波, 评估浙江省台网丘陵地带基岩台站场地效应, 计算穿越台湾海峡较单一路径Lg波衰减参数. 研究使用20次发生于2002——2005年、 震级在MS5.0~6.7之间的台湾东北部较小区域地震, 参与评估台站16个, 地震波记录960条. 地震波处理频段为0.5~10.0 Hz, 每间隔0.2 Hz计算一次,对应于垂直、 东西及南北分量获得的衰减参数, 数据结果分别为:gamma;(f )=0.001 75f 0.43485, gamma;(f )=0.001 45f 0.48467, gamma;(f )=0.0021f 0.41241. 庆元台(QIY)在1.5 Hz以上放大效应非常明显,宁波台(NIB)在大部分频率点场地效应最小,参与评估台站场地效应各分向基本相当,未表现出方向性特征.   相似文献   

7.
采用Nakamura方法,利用2007年6月3日宁洱地震强震动记录S波资料和脉动观测资料,计算了宁洱震区一些强震动台的场地响应.结果表明,当台站场地为基岩或覆盖层较薄时,由脉动数据和S波数据分别计算的谱比曲线一致性很好.当覆盖层大于35 m的时候,两者的谱比值有差异,即用S波计算的场地放大响应要明显大于用脉动计算的场地响应.  相似文献   

8.
用广义反演方法估算了阿拉斯加州中南部安克雷奇盆地场地响应(SR)的空间变化。所分析资料表现的是近震S波水平分量记录的弱运动。数据资料是来自22个便携式临时台站(采用IRIS-PASSCAL仪器)大约6个月时间运行的记录。选定相对每个地震震源到台站的路径效应,然后对数据进行反演确定场地响应值。对所得到的场地响应按2个频段分别求(对数)平均值,一个低频段(LFB),频率从0.5到2.5Hz和一个高频段(HFB),频率从3.0到7.0Hz,低高频段的中心频率分别大约是1.0Hz和5.0Hz。在低频段,场地响应值沿着东部的楚加奇山丘陵从1.0增加到西部的坎贝尔湖和首府山及其周围地区的3.5左右。场地响应值大于3.0的区域与1964年威廉王子海峡地震(Mw=9.2)中广阔的破坏区相关联。在高频段,安克雷奇南边有两个场地响应值大于3.0的小区域连接着特纳甘湾。把用广义反演方法获得的场地响应值与其他研究方法获得的结果进行了对比。结果表明,广义反演法的场地响应值与标准谱比率法(SSR)获得的值大致相当(1∶1),水平与垂直向谱比率法(HVR)获得的场地响应值是广义反演法获得的场地响应值的2倍。研究还发现,在低频段,D级土壤地区的场地响应值SR>2.0,而C级土壤地区的场地响应值SR≤2.0,但在高频段,没有得到土壤类别与场地响应值的关系。  相似文献   

9.
基于强震观测记录,采用广义反演法和HVSR法分析日本仙台盆地48个强震台站以及场地vS30和盆地深度对放大效应的影响。研究表明,相比于广义反演法,HVSR法能够较好地给出场地主频,但会明显低估放大效应的幅值;处于盆地外不同位置的浅源地震引起的盆地放大效应差异明显,仙台盆地南部海域地震引起的放大效应最大,盆地北部陆地地震引起的放大效应最小;盆地南部和东部地震引起的S波的放大效应与vS30的相关性较强,北部地震的放大效应与vS30基本不相关;盆地S波的放大效应与盆地深度在0.5~5 Hz频段内的相关性较强,在0.25~0.5 Hz和5~10 Hz频段内基本不相关。  相似文献   

10.
安徽强震动台站场地响应研究   总被引:1,自引:0,他引:1  
采用H/V谱比法,利用安徽强震台网记录的波形数据,计算了3个强震台的场地响应。结果表明,当台站场地为基岩或覆盖层较薄时,由地脉动和S波数据分别计算出的谱比曲线一致性很好。当覆盖层大于30.5 m的时候,两者的放大因子有差异,即用S波计算的场地放大响应要明显大于用脉动计算的场地响应。  相似文献   

11.
江苏地区介质非弹性衰减和场地响应研究   总被引:1,自引:0,他引:1  
选取江苏数字地震台网在2001年1月-2010年7月记录到43次高质量数字地震波形,采用Atkinson(1992)和Moya(2000)的方法,反演得到江苏地区的介质非弹性衰减特性和场地响应.  相似文献   

12.
We have explored 1D S-wave velocity profiles of shallow and deep soil layers over a basement at strong motion stations in Eskisehir Province, Turkey. Microtremor array explorations were conducted at eight strong motion stations in the area to know shallow 1D S-wave velocity models. Rayleigh wave phase velocity at a frequency range from 3 to 30 Hz was estimated with the spatial autocorrelation analysis of array records of vertical microtremors at each station. Individual phase velocity was inverted to a shallow S-wave velocity profile. Low-velocity layers were identified at the stations in the basin. Site amplification factors from S-wave parts of earthquake records that had been estimated at the strong motion stations by Yamanaka et al. (2017) were inverted to the S-wave velocities and Q-values of the sedimentary layers. The depths to the basement with an S-wave velocity of 2.2 km/s are about 1 km in the central part of the basin, while the basement becomes shallow as 0.3 km in the marginal part of the basin. We finally discussed the effects of the shallow and deep sedimentary layers on the 1D S-wave amplification characteristics using the revealed profiles. It is found that the shallow soil layers have no significant effects in the amplification at a frequency range lower than 3 Hz in the area.  相似文献   

13.
Butterworth band-pass filter has been applied to S-wave data recorded at 8 stations in China mainland, and S-wave splitting at different frequency bands is analyzed. The results show that the delay time and the fast polarization directions of S-wave splitting depend upon the frequency bands. There is an absence of S-wave splitting at the station of Urumqi (WMQ) for the band of 0.1–0.2 Hz. With the frequency band broadening, the delay time of S-wave splitting decreases at the stations of Beijing (BJI), Enshi (ENH), Kunming (KMI) and Mudanjiang (MDJ); the fast polarization direction changes from westward to eastward at Enshi (ENH), and from eastward to westward at Hailaer (HIA). The variations of delay time with bands at Lanzhou (LZH) and Qiongzhong (QIZ) are similar, and there is a coherent trend of fast polarization directions at BJI, KMI and MDJ, respectively. Initial interpretations to the results of frequency band-dependence of S-wave splitting are also presented.  相似文献   

14.
Introduction It has been known that each soil type responds differently when it is subjected to ground mo-tion from earthquakes. So, the study of local site effects on seismic ground motions is one of the most important goals of earthquake engineering. It is practical importance to develop methods for assessing the nature and potential of sediment amplification, especially when choosing the location and design of critical and essential facilities. At present, however, the method by which site …  相似文献   

15.
Simultaneous estimation of effects of source, propagation path, and local site amplification was carried out using observed strong motion records in a frequency range from 0.8 to 20 Hz for the purpose of empirical evaluation of the local site effects in different geological conditions in the northwestern part of Turkey. The analyzed data are S-wave portions of 162 accelerograms from 39 shallow events observed at 14 sites of BYTNet array. A spectral separation method was applied to the observed S-wave spectra. The solutions for source spectra, inelasticity factor of propagation path for S-waves (Q s-value), and factor of site amplification at each site were obtained in a least squares sense. In the analysis, we assumed that the factor of the site amplification at a reference site is the same as that of theoretical amplification of S-waves to the soil model whose bottom layer has an S-wave velocity around 2.15 km/s. The estimated Q s-value of the propagation path is modeled as Q s(f)?=?87.4f0.78. The estimated site amplifications are characterized into three groups. The sites in the first group belong to rock site with no dominant peaks at a frequency range of 2 to 10 Hz. The second group of hard soil sites is characterized with moderately dominant peaks at a frequency of 5 Hz. The last group for soft soil sites has common peaks at a frequency of 4 Hz with larger amplitudes than those in the hard soil group. We, then, compare the amplifications with average S-wave velocity in top 30 m of the shallow S-wave profiles and proposed linear empirical formula between them at each frequency. We, furthermore, inverted the observed amplification factors into S-wave velocity and Q s-value profiles of the deep soil over the basement.  相似文献   

16.
利用乳山流动地震台网记录的2013年10月1日乳山M_L 3.8震群资料,基于Atkinson方法,计算得到该区Q值与频率f的关系:Q(f)=57.8 f ~(0.8562)。Moya方法仅依赖震源模型,计算绝对场地响应值,较能反映实际放大效应。采用该方法,计算14个流动地震台站场地响应,结果显示,场地响应在低频(1—2 Hz)放大作用不明显,而高频部分平均放大2—10倍,卓越频率3—10 Hz,且高频处场地响应衰减不明显。  相似文献   

17.
The generalized inversion of S-wave amplitude spectra from the free-field strong motion recordings of the China National Strong Motion Observation Network System (NSMONS) are used to evaluate the site effects in the Wenchuan area. In this regard, a total of 602 recordings from 96 aftershocks of the Wenchuan earthquake with magnitudes of M3.7-M6.5 were selected as a dataset. These recordings were obtained from 28 stations at a hypocenter distance ranging from 30 km to 150 km. The inversion results have been verified as reliable by comparing the site response at station 62WUD using the Generalized Inversion Technique (GIT) and the Standard Spectral Ratio method (SSR). For all 28 stations, the site predominant frequency F p and the average site amplification in different frequency bands of 1.0–5.0 Hz, 5.0–10.0 Hz and 1.0–10.0 Hz have been calculated based on the inversion results. Compared with the results from the horizontal-to-vertical spectral ratio (HVSR) method, it shows that the HVSR method can reasonably estimate the site predominant frequency but underestimates the site amplification. The linear fitting between the average site amplification for each frequency band and the V s20 (the average uppermost-20 m shear wave velocity) shows good correlation. A distance measurement called the asperity distance D Aspt is proposed to reasonably characterize the source-to-site distance for large earthquakes. Finally, the inversed site response is used to identify the soil nonlinearity in the main shock and aftershocks of Wenchuan earthquake. In ten of the 28 stations analyzed in the main shock, the soil behaved nonlinearly, where the ground motion level is apparently beyond a threshold of PGA > 300 cm/s2 or PGV > 20 cm/s, and only one station coded 51SFB has evidence of soil nonlinear behavior in the aftershocks.  相似文献   

18.
姜秀璇  郭晓  范兵  邹锐 《地震工程学报》2021,43(6):1343-1351
场地响应是精确测定震源参数和稳健估计出高精度地壳介质衰减变化的关键影响因素之一,采用H/V尾波谱比法,对祁连山主动源观测台网中40个短周期观测台站的场地响应进行了分析。结果表明,祁连山主动源观测台网中40个短周期观测台站均存在不同程度的放大(衰减)作用,根据40个台站观测波形的尾波场地响应曲线特征,可将其分为平坦类、放大类、高频衰减类,在1~20 Hz频段内部分台站场地响应曲线呈现平坦,场地响应值为1~2倍;而大部分台站在不同频段有明显放大(衰减)作用,场地响应值为0.3~9倍。台站台基岩性可能是决定场地响应曲线特征和大小的主要因素,且与台基介质密度具有反相关性。  相似文献   

19.
Introduction Located between Qingzang (Qinghai-Xizang) Plateau that highly uplifts due to compression and North China plain that badly subsides due to crustal extension, the Ordos massif has both the basic attributes of stretching tectonic region of North China marginal basin and the features of marginal shear-compression zone of Qingzang Plateau. It has a length of about 600 km in the N-S direction and a width of about 400 km in the W-E direction. Its geological structure is very simple…  相似文献   

20.
利用不同方法估算流动台站的场地响应   总被引:5,自引:0,他引:5  
华卫  陈章立  郑斯华 《地震》2010,30(3):30-44
本文以2003年7月21日云南大姚6.2级地震序列为例, 分别利用地面运动反演法(Moya方法)、 水平与垂直向之比法(Nakamura方法)和参考台站法研究大姚地区场地响应特征。主要结论有: ① Moya方法计算的场地响应结果表明, 大姚地区场地的放大作用是比较明显的, 平均在3~20倍, 最高达到40倍; 卓越频率位于3~6 Hz之间, 但在高频处(约10 Hz以上)场地响应衰减得比较明显; 不同岩性台基的台站, 其场地响应结果存在一定的差别, 台基为风化砾岩的场地响应结果比较平缓, 其场地响应值比台基为土层的其他台站小一些。② 入射角在40°以上和以下范围, Nakamura方法得到的场地响应形态有差异, 但在各自范围内, 场地响应与入射角的依赖关系不明显。③ 利用同一台站不同时间记录到的地震资料, 由三种方法各自得到的场地响应都具有较好的稳定性; 由于垂直分量仍具有放大作用(在10 Hz以下), Moya的结果大于Nakaruma的结果, 但两者形态上一致性较好; 参考台站法由于受参考台站的影响, 计算得到的场地响应形态和其他两种方法差异较大。④ Moya方法是依赖于震源模型的方法, 它能给出绝对的场地响应值, 其它两种方法的结果是一种相对场地响应, 受参考对象的影响较大。  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号