云南地区尾波衰减特征研究     

王伟君  刘杰  陈凌 《地震学报》2006,28(1):8-19

利用22个云南区域数字地震台网近震资料,研究了云南地区地震尾波在1~20 Hz内6个频段的衰减特征. 首先使用单次散射模型计算各台站的尾波衰减系数; 然后利用随机各向同性散射介质均匀分布的多次散射模型, 使用多流逝时间窗分析方法,计算各台站的平均自由程Le和地震反照率B0得到总衰减系数,并从中分离散射衰减系数 、吸收衰减系数 . 云南地区基本衰减特征是Le主要集中在10~30 km内, 在2~6 Hz之间有最大值;B0在1~2 Hz大致为0.5左右,在其它频段则小于0.5. 也即在1~2 Hz, 与 数值相当, 其它频段 逐渐大于,成为尾波总衰减的主要原因. 除1~2 Hz外,其它频段 值接近. 云南地区的Q-1尤其是, 在空间上有较大的差异,滇东略微高于滇西北, 滇西北高于滇西南地区. 与全球其它区域的研究结果比较发现,云南地区 略低于平均水平, 略高于平均水平, 而则处于其它区域结果的中间.   相似文献   

地壳介质破裂的尺度理论在研究山丹-民乐 6.1级地震的地震学前兆特征中的应用   总被引：2，自引：0，他引：2       下载免费PDF全文

荣代潞  李亚荣  韩晓明 《地震学报》2006,28(4):438-447

介绍了Allegre的地壳介质破裂的尺度理论和根据该理论建立一种预测地震发生时间方法的可能性. 作为震例研究了甘肃山丹——民乐6.1级地震的地震学前兆（地震空间相关长度和尾波Qc值）特征. 结果表明,地震空间相关长度和尾波Qc值在震前都呈增长趋势,用幂次率关系拟合了这两种参数的上升变化形态. 这为利用地震空间相关长度和尾波Q值的监测资料建立一种预测地震发生时间的方法和找到预测指标打下了基础.   相似文献   

依舒断裂带北段尾波Q值特征研究     

李继业  孙鹏宇  武晓军  张彦吉  任建辉  秦丽岩  孙强 《中国地震》2018,34(3):545-550

研究表明,地震波穿过构造活动相对稳定地区时,能量衰减不明显且具有高Q值;而穿过构造活动地区时,能量会发生强烈衰减且具有低Q值。本文利用Sato模型对依舒断裂带北段萝北-通河地区15个数字化地震台站记录到的266条M_L≥2.0地震尾波Q_c值进行了分析和研究,发现黑龙江萝北、通河附近地区Q_c值具有明显的复杂性和差异性,且萝北地区Q_c值远低于通河地区Q_c值,其原因一方面与区域构造活动有关,另一方面与区域地壳构造复杂、地下介质破碎、区域应力不断变化有关。本文还讨论了萝北、通河附近地区Q值随着频率变化的关系及Q_0值空间分布特征,有效地分析了该区域介质状态的变化过程,对萝北地区地震活动性的研究和预测有指导意义。  相似文献   

Crustal scattering at the KTB from a combined microearthquake and receiver analysis     

Andreas Rietbrock  & Frank Scherbaum 《Geophysical Journal International》1999,136(1):57-67

In December of 1994 a fluid injection experiment which triggered several hundreds of microearthquakes was conducted at the KTB main borehole (Oberpfalz, Germany). These events were recorded with a temporal seismic network at the surface. Out of the complete data set, a cluster of five events recorded at four mini-arrays consisting of eight or nine stations was used to investigate the crustal scattering properties in the vicinity of the KTB. For this purpose, the 'Double Beam Method' (DBM; Krüger et al . 1993 , 1995 , 1996) and the 'Double Beam Imaging Method' (Scherbaum, Krüger & Weber 1997) were extended to curved wave fronts to drop the restriction of plane-wave propagation. This technique is used for imaging the crustal scattering strength using earthquake clusters recorded at close-by mini-arrays. The results of the array analysis show that the composition of the P coda is mainly affected by the site location of the arrays. Near-surface and deeper crustal scattering contribute in a very complicated pattern. Furthermore, with the present data set it was possible to identify reflections from the top of the Erbendorf Body. This is a very pronounced arrival in most of the recorded traces. In one of the arrays its amplitudes are even greater than the direct P phases. Five to eight coherent phases could be identified by the mini-arrays. Using only these phases, synthetic P -coda traces were constructed, which only contain the coherent part of the observed wavefield. By subtracting the synthetic coherent wavefield from the original traces we achieve a variance reduction in the P coda of up to 37 per cent. This leads to the conclusion that a large amount of the P coda at the KTB can be modelled by a simple deterministic single-scattering model using a small number of individual scatterers.  相似文献   

Residence time of diffuse waves in the crust as a physical interpretation of coda Q: application to seismograms recorded in Mexico   总被引：4，自引：0，他引：4  

L. Margerin  M. Campillo  N. M. Shapiro  & B. van Tiggelen 《Geophysical Journal International》1999,138(2):343-352

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The physical implication of coda amplitude ratio and its possible application     

Tian-Zhong Zhang  Yun-Sheng Ma  Rong-Liang Huang 《地震学报(英文版)》1998,11(4):441-448

The physical implication of coda amplitude ratio is discussed in term of energy ratio. The digitized data recorded at the station of Beijing Telemetered Seismograph Network between 1989 and 1990 are used to calculate amplitude ratios of coda to direct S wave, and energy ratios. The spectral energy ratios are used to estimate the coda Q and mean free path l in the Beijing area, as well as the two quality factors Q _i and Q _S separately due to intrinsic absorption and scattering attenuation. The decay of seismic waves in their propagation seems mainly resulted from the intrinsic absorption in Beijing region. The temporal variations of amplitude ratio and energy ratio at Changli station during the above two years are inspected; some of them largely depart from their mean value. It may reflect the seismogenic process, but using the data lasting longer time with more case histories needs further study. This study is sponsored by the Key Project of State Science and Technology of China, No. 96-918.  相似文献   

Constituents of Vertical-component Coda Waves at Long Periods     

Takuto Maeda  Haruo Sato  Masakazu Ohtake 《Pure and Applied Geophysics》2006,163(2-3):549-566

Aki (1969) first modeled coda waves of a local earthquake as a superposition of scattered surface waves. This paper attempts to clarify the constituents of surface-wave coda at long periods at very long lapse times. For a large earthquake of magnitude 7 or larger, vertical component oscillation in periods from 90 to 180 s persists for more than 20 hours from the earthquake origin time. Although the early portion of the coda envelope is successfully modeled by assuming incoherent scattered Rayleigh waves by heterogeneities distributed all over the Earth, the later potion of the observed coda envelope (roughly later than 35,000 s) has systematically larger amplitude than theoretical prediction. To clarify the cause of this discrepancy, we studied the constituents of vertical-component seismograms of three large earthquakes recorded by the F-net in Japan using the f-k power spectral analysis. We found that the direct and scattered fundamental-mode Rayleigh waves of velocity about 3.7 km/s are dominant in the earlier part of each envelope. It justifies the use of a scattering model of the fundamental Rayleigh waves for synthesizing the envelope. At lapse times later than 20,000 s–35,000 s, higher modes with phase velocities around 20 km/s become dominant. The transition time to the dominance of higher modes is found to become earlier for a deeper focus earthquake. The small coda attenuation factor from (1.90±0.23) × 10⁻³ to (2.38±0.32) × 10⁻³ estimated from later coda envelopes recorded at IRIS stations distributed worldwide also agrees with the attenuation factor of spheroidal modes according to PREM. We may interpret that higher mode waves are uniformly distributed at large lapse time due to large velocity dispersion and/or scattering and they dominate over the fundamental mode waves because of smaller attenuation in the lower mantle. The coda attenuation measurement proposed by Aki is found to be useful even for long periods and at very large lapse times.  相似文献   

云鹏水电站及其周围地震尾波Q_c值研究     

赵小艳  付虹  毛玉平  邬成栋 《地震研究》2010,33(1)

利用云鹏水电站周边5个数字地震台站记录到的2000年1月至2008年12月间的108个地震的数字波形资料,采用Aki单次散射模型,计算了各台站周围423条地震记录的尾波Q0值。结果显示:云鹏水电站地区尾波的Qc值与频率的关系为Qc(f)=90.2f0.94。该地区的Q0值比云南其它构造活动强烈地区的要高,因此属于中等构造活动地区。云鹏水电站蓄水后弥勒台记录到的108个地震的尾波Q0值及分频Qc值有所下降,但下降幅度不大,表明水库蓄水对库区及其附近区域地下介质性质有所影响,但影响的程度有限。  相似文献   

利用两种模型对宁夏及邻区尾波 Q 值进行对比研究   总被引：1，自引：0，他引：1  

贺永忠  师海阔  朱新运  张立恒 《大地测量与地球动力学》2012,32(Z1):10-17

分别利用Aki模型和Sato模型,选取2008年1月-2009年12月宁夏地震台网记录的ML≥2.0地震的数字地震波资料,计算了宁夏及邻区平均尾波Q值,并拟合了Q值对频率的依赖关系.结果为:Aki模型为Q(f)=(212±87.62)f0.7584±0.19;Sato模型为Q(f)=(44.81±15.87)f0.9491±0.0805.与国内其他区域相比,两种模型计算结果均显示本区域Q值较低,对频率依赖性较高.研究结果认为两种模型均适合对宁夏及邻区尾波Q值的研究.  相似文献   

利用Sato模型研究上海及邻近地区尾波Q值     

陈婧  赵文舟 《地震地磁观测与研究》2015,(1)

利用2011年至2013年上海及邻近地区的常熟地震台、金泽地震台、佘山地震台记录的ML2.0以上地震波资料,基于Sato模型,采用不同的流逝时间,计算该区域的尾波Q值。结果表明:该区域为低Q值、高频率依赖性区域;不同流逝时间下同一个地震的Q值是不同的,流逝时间越长Q值越大;在2012年7月20日江苏宝应ML5.0级地震发生前,尾波Q值存在增大现象。  相似文献