共查询到19条相似文献，搜索用时 187 毫秒
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根据eQuake-RC网站及相关文献,建立了383个地震全局参数的数据集,与二十多年中3篇参考文献先后发表的震源全局参数及其定标律统计结果比较,讨论了定标律的稳定性。虽然数据量大大增加,尤其是高震级数据增加更显著,震级范围扩大,不同年代的全局参数与矩震级域数据点的分布大多重叠,新补充的数据往往分布在以往数据分布的延伸方向上。区分两类地震、三种破裂类型、五(三)个震级段统计全局参数定标律,与3篇参考文献的结果比较,期望值两两相对差别的特征相近,统计标准差有所减小,说明随数据增加全局参数定标律结果变化不大,总体趋于稳定。分4组比较、分析数据分布的区域特征,没有发现系统性差别,说明全球数据是可以一起统计的。板内地震和俯冲带地震分组的结果表明,震级范围不同,高震级段数据分布存在明显差异,宜分开统计。 相似文献
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3.
在进行未来破坏性地震的强地面运动数值模拟时,震源参数选取的准确性对地震动预测的结果影响很大。震源参数的确定存在很多不确定性因素,既包含随机的不确定性因素,又包含认知的不确定性因素。本文在大量地震事件及文献调研的基础上,运用统计学方法对具备随机不确定性特征的震源参数进行统计研究,以震源参数经验公式的形态建立解释其随机性和不确定性的数学模型。为了研究局部地区震源参数的定标关系特征,获得更加适用于局部地震密集区域,尤其是包含中国大陆地区在内的局部区域的震源参数的经验关系,本文从GCMT地震目录中选取了1 700多个MW≥5.5的地震事件,运用统计学方法研究地震密集地区的震源参数经验关系,包括震级、地震矩、破裂面积等,增加了相对较大的局部范围内凹凸体的地震样本数量,从统计学角度计算更加适合局部区域的震源参数的经验关系。统计结果表明:局部区域震例获得的震源参数的经验关系与不限区域震例获得的经验关系存在差异,尤其是涉及到断层破裂面积、凹凸体相关参数时差异较大,局部区域内震例获得的震源参数的经验关系将更具有代表性。应用本文获得的相对局部区域的经验公式计算未来破坏性地震的强地面运动所需的震源参数时,获得的地震动预测结果将更能体现目标区域真实的地震动特征,进而提高地震动预测结果的可靠性。 相似文献
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区域地震波形对于震源研究非常重要,但限幅问题限制了区域地震台网数据的运用,并影响到震源参数测定的准确度.本文利用恢复后的芦山地震区域地震波形,研究了芦山地震的震级、点源机制解以及破裂过程.基于震中距99~300 km恢复前与恢复后地震数据获取的面波震级分别为7.01与7.06级.分别利用7个震中距150~250 km宽频带台站的恢复前和恢复后的数据反演点源机制解,与参考机制解相比,滑动角偏差自13°减小到了4°.基于7个震中距81~134 km的区域地震波形联合远场数据获得的震源破裂过程结果,其主要参数（如滑动分布、破裂速度等）与强地面运动波形联合远场数据得到的结果具有很好的一致性.研究结果表明,本文所采用的数据恢复方法具有较高的可靠性,有效提高了震源参数测定的准确度. 相似文献
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《地震工程与工程振动》2017,(6)
从eQuake-RC的有限断层源破裂模型数据库等来源收集、整理了全球范围的211个地震的错动分布,逐一从中提取局部震源参数,区分板内地震和俯冲带地震,建立了三种破裂类型的凹凸体参数,包括最大凹凸体和其它凹凸体的面积、长度,平均错动量,凹凸体中心和破裂起始点的坐标等与相应全局参数的定标律。经过对比分析,发现凹凸体参数与全局参数关系比与矩震级关系的离散性和相对误差都小得多。与相关文献的结果比较,由于本文数据量的大幅度增加,得到的有限断层模型局部参数定标律的可靠性有很大提高。 相似文献
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《四川地震》2014,(3)
本文根据2009年10月以来,江苏省及附近海域ML≥2.8级地震的地震波形观测数据,运用快速傅里叶变换方法对地震S波数据进行地震波位移谱和震源参数计算,并将江苏区域测震台网内部分地面测震观测得到的震源参数与井下观测得到的震源参数进行归纳对比,发现地面观测的地震震源参数中的拐角频率、地震矩和断层错动距离、应力降和矩震级要大于井下观测的震源参数结果,拐角频率f0差值为0.397 Hz、地震矩M0差值为8.642×1014 N·m、断层错距的差值为2.268 cm、应力降差值为2.033 MPa,矩震级差值为0.32级。而地面观测计算出的断层错动尺度参数和断层破裂面积参数要小于井下观测数据计算的结果,两者的差值分别是-0.126 km和-0.221 km2。 相似文献
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地震发生后,针对能够快速预测震中附近的烈度分布情况的问题,首先对632次地震触发的台站进行筛选,对2 231个台站触发后20 s内有效的7个地震动参数以及震级和震源距的信息进行提取,并利用人工神经网络对所选数据样本进行训练,建立三种有效的预测模型。研究结果显示模型一所选的输入参数为7个,不利用震源参数,在预测中有着较好的时效性,从第1 s到20 s,预测的平均烈度差值逐渐减小到0.45;模型二所选的输入参数为8个,利用了震源距信息,可以用于烈度级别的预测,预测的平均烈度差值逐渐减小到0.36;模型三所选的输入参数为9个,预测结果较好,可用于震后烈度场的实时预测,平均烈度差值逐渐减小到0.31。利用提出的3种模型对两次地震事件进行烈度预测,预测烈度差值取整后分别有95%和76%以上在1以内,有着较好的结果,可以用于地震预警当中。 相似文献
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研究震源参数与震级之间的定量关系停留在相关统计上是不够的。震源参数与震级之间可能存在着确定性的函数关系(物理关系)。本文利用76个云南地震(4.0≤M_s≤5.8)数据,得到了一组互相一致的云南地震震源参数与面波震级 M_s 的函数关系:M_s=lgM_o-lgr-17.94 s=±0.32M_s=lg△σ+lgA+2.92 s=±0.33M_s=lg(?)+lgr+4.04 s=±0.33式中地震矩 M_o、地震应力降△σ、震源破裂面半径 r、面积 A 及平均断错(?)的单位,分别为达因·厘米、巴、公里、平方公里和厘米。s 为剩余标准差。 相似文献
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传统地震目录中增加矩震级及震源机制解的必要性分析 总被引：1，自引：0，他引：1
本文梳理了我国地震目录的产出现状,对于我国近几年应急机构和区域台网产出的震源机制解、矩震级进行了比较研究。结果表明:中国地震局地球物理研究所和地震预测研究所对于国内陆地地区6级以上地震的地震矩张量解的产出率为100%,5级以上地震的地震矩张量解产出率为81%。这两个研究所给出的3种矩张量结果和GCMT给出的矩张量结果较为一致,类型统计一致率分别达到71%、86%和66%,其中P、T轴空间夹角优势分布在15°左右。产出的矩震级和GCMT解得到的矩震级相差不大,偏差在0.1以内的比率分别为46%、86%和71%,偏差在0.3以内的比率分别为85%、100%和97%。结果表明对于我国内陆地区的5级以上地震,这两个研究所产出率较高、结果较为一致。而由各台网据震源参数得出的5级左右地震的矩震级和GCMT求解的矩震级比较起来明显偏小。由此探讨了在传统地震目录中增加震源机制解及矩震级的必要性。 相似文献
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本文根据建立在平均二维破裂模式基础上的地震定标律,导出了地震矩 M0与各常用震级之间（1gM0-MS,ML,mb）,各种震级之间（Ms-ML,Ms-mb,ML-mb）,各震源参数之间（断层长度IgL,断层面积 lgS,平均错距 lgD-Ms,拐角频率 1gfc-ML）的各种常用的关系式.利用这些关系式,由一个震级值就可以估算出一系列震源参数.本文还求出了平均破裂速度 Vr=2.65km/s,总破裂时间 T（s）=0.5L（km）,平均位错速度 D（t）=11.4m/s.用矩震级 Mw 度量地震的大小,有四个优点:（1）地震矩反映了形变规模的大小,因此是度量地震大小的最佳物理量.（2）它是一个绝对力学标度,对任何大小地震都有意义,可测量,且不产生饱和问题.（3）它和我们已熟悉的震级标度可衔接.（4）它是一个均匀的震级标度,适用于宽尺度的地震统计.因此,Mw 是一种值得推广的震级标度. 相似文献
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1 Introduction Earthquake disaster investigations show that numerous strong earthquakes were caused by remobilization of active faults. Major casualties and severe damage to buildings as well as signi?cant economic losses resulted from the ground motions of strongearthquakescausedbyactivefaultslocatedbeneath urban areas. Recently, the potential hazard prediction of and its mitigation against active faults located beneath urban areas have become an important research topic for seismologists and… 相似文献
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《Geofísica Internacional》2014,53(2):211-220
We apply a single-step, finite-fault analysis procedure to derive a coseismic slip model for the large MW 7.4 Ometepec-Pinotepa Nacional, Mexico earthquake of 20 March 2012, using teleseismic P waveforms recorded by the Global Seismographic Network. The inversion is conducted in near-realtime using source parameters available from the USGS/NEIC and the Global Centroid Moment Tensor (gCMT) project. The fault orientation and slip angle are obtained from the gCMT mechanism assuming that the fault coincides with the shallow-dipping nodal plane. The fault dimensions and maximum rise time are based on the magnitude reported for the event. Teleseismic data from the USGS/NEIC Continuous Waveform Buffer database are used in the inversion with record start times set to the P-wave arrivals used to compute the earthquake hypocenter. The inversion is stabilized by requiring a smooth transition of slip across the fault while minimizing the seismic moment. These constraints are applied using a smoothing weight that is estimated from the inverse problem, allowing the recovery of the least-complicated rupture history in a single step. Inversion of the deconvolved, ground-displacement waveforms reveals a simple, circular rupture similar in extent to the source identified by the USGS/NEIC using body-and surface-wave data, indicating that the teleseismic P waves can provide a first-order source model for the event in near-realtime. Additional inversions conducted using velocity records identify a more-detailed rupture model characterized by an elliptical 2500 km2 source region extending updip and downdip from the hypocenter. This elliptical source preserves the orientation and overall dimensions of a dual-source slip model obtained recently by other investigators using local strong motions and global seismic waveforms. The results indicate that velocity waveforms could provide additional details of the earthquake rupture in near-realtime, finite-fault inversions using teleseismic P waves. 相似文献
13.
A simple hybrid approach for the simulation of strong ground motion is presented in this paper. This approach is based on
the deterministic modelling of rupture plane initially started by Midorikawa, Tectonophysics 218:287–295, (1993) and further
modified by Joshi, Pure Appl Geophys (PAGEOPH) 8:161, (2004). In this technique, the finite rupture plane of the target event
is divided into several subfaults, which satisfy scaling relationship. In this paper, simulation of strong ground motion due
to a rupture buried in a earth medium consisting of several layers of different velocities and thicknesses is made by considering
(1) transmission of energy at each layer; (2) frequency filtering properties of medium and earthquake source; (3) correction
factor for slip of large and small magnitude earthquakes and (4) site amplification ratio at various stations. To test the
efficacy of the developed technique, strong motion records were simulated at different stations that have recorded the 2004
Niigata-ken Chuetsu, Japan earthquake (M
s 7.0). Comparison is made between the simulated and observed velocity and acceleration records and their response spectra.
Distribution of peak ground acceleration, velocity and displacement surrounding the rupture plane is prepared from simulated
and observed records and are compared with each other. The comparison of synthetic with the observed records over wide range
of frequencies shows that the present technique is effective to predict various strong motion parameters from simple deterministic
model which is based on simple regression relations and modelling parameters. 相似文献
14.
This paper presents a novel approach to identify the pulse-like motions in earthquake recordings that dominate the maximum structural responses over a wide period range. The identification method is based on the congruence relationship between the response spectrum and the dimensionless П-response spectrum established in this study through straightforward dimensional arguments of linear and bilinear SDOF oscillators subject to pulse-like ground motions. By evaluating the geometric match and dislocations of the П-response spectrum of a given waveform with the dimensional response spectrum in bi-logarithm plotting, one can identify the simple pulses and their parameters that match simultaneously the kinematic characteristics and the response spectrum of earthquake recordings that exhibit pulse-like features. The developed pulse identification method has been implemented in a computer program and applied successfully to detect the pulse-like motions in the PEER NGA strong motion database. Both velocity and acceleration pulses potentially due to forward directivity effects in near fault regions are identified. The identified velocity pulses show strong correlation with the seismological parameters. They are subsequently used in regression analysis to derive the empirical scaling laws that relate the directivity pulse parameters to the earthquake magnitude and rupture distance. The study confirms some magnitude scaling laws in literature and demonstrates the accuracy and efficiency of the proposed pulse identification method. 相似文献
15.
In the analysis and design of important structures with relatively long life spans, there is a need to generate strong motion data for possible large events. The source of an earthquake is characterized by the spatial distribution of slip on the fault plane. For future events, this is unknown. In this paper, a stochastic earthquake source model is developed to address this issue. Here, 1D and 2D stochastic models for slip distribution developed by Lavallée et al.(2006) are used. The random field associated with the slip distribution is heavy-tailed stable distribution which can be used for large events. Using 236 past rupture models, the spectral scaling parameter and the four stable or Levy's parameters against empirical relationship for known quantities like magnitude or fault length are developed. The model is validated with data from 411 stations of 1999 Chi-Chi earthquake. The simulated response spectrum showed good agreement to actual data. Further the proposed model is used to generate ground motion for the 1993 Killari Earthquake where strong motion data is not available. The simulated mean peak ground velocity was in turn related to the intensity(MSK) and compared against values in the literature. 相似文献
16.
Comparison of source parameters estimated in the frequency and time domains for seismic events at the Rudna copper mine,Poland 总被引：3，自引：0，他引：3
Source parameters estimated in the frequency domain for 100 selected seismic events from the Rudna copper mine, with moment
magnitude ranging from 1.4 to 3.6, were collected to study their scaling relations and to compare them with the parameters
estimated in the time domain. The apparent stress and static stress drop, corrected for the limited bandwidth recording, increase
slightly in a similar manner with increasing seismic moment. The ratio of apparent stress to static stress drop, a measure
of radiation efficiency, is practically constant and its mean value is close to 0.1.
For 37 seismic events, with moment magnitude between 1.9 and 3.4, source parameters were estimated in the time domain from
relative source time functions, that displayed unilateral rupture propagation, and their rupture velocity could be estimated.
It ranges from 0.23 to 0.80 of shear wave velocity and is almost independent of seismic moment. The fault length, estimated
from the average source pulse width and rupture velocity, is clearly dependent on seismic moment and is smaller than the source
radius estimated from the corner frequency on the average by about 25 percent. There is no correlation between the values
of static stress drop estimated in the frequency and time domains, but the time domain stress drop is in general similar to
that estimated in the frequency domain. The apparent stress increases with increasing rupture velocity, and the ratio of apparent
stress to static stress drop seems also to depend on rupture velocity. 相似文献
17.
Relationships between moment magnitude and fault parameters: theoretical and semi-empirical relationships 总被引：1，自引：0，他引：1
Fault parameters are important in earthquake hazard analysis. In this paper, theoretical relationships between moment magnitude and fault parameters including subsurface rupture length, downdip rupture width, rupture area, and average slip over the fault surface are deduced based on seismological theory. These theoretical relationships are further simplified by applying similarity conditions and an unique form is established. Then, combining thc simplified theoretical relationships between moment magnitude and fault parameters with seismic source data selected in this study, a practical semi-empirical relationship is established. The seismic source data selected is also to used to derive empirical relationships between moment magnitude and fault parameters by the ordinary least square regression method. Comparisons between semi-empirical relationships and empirical relationships show that the former depict distribution trends of data better than the latter. It is also observed that downdip rupture widths of strike slip faults are saturated when moment magnitude is more than 7.0, but downdip rupture widths of dip slip faults are not saturated in the moment magnitude ranges of this study. 相似文献
18.
In seismological literature, there exist two competing theories (the so-calledW model andL model) treating earthquake scaling relations between mean slip and rupture dimension and between seismic moment and rupture dimension. The core of arguments differentiating the two theories is whether the mean slip should scale with the rupture width or with the rupture length for large earthquakes. In this paper, we apply the elastic theory of dislocation to clarify the controversy. Several static dislocation models are used to simulate strike-slip earthquakes. Our results show that the mean slip scales linearly with the rupture width for small earthquakes with a rupture length smaller than the thickness of the seismogenic layer. However, for large earthquakes with a rupture length larger than the thickness of the seismogenic layer, our models show a more complicated scaling relation between mean slip and rupture dimension. When the rupture length is smaller than a cross-over length, the mean slip scales nearly linearly with the rupture length. When the rupture length is larger than a cross-over length, the mean slip approaches asymptotically a constant value and scales approximately with the rupture width. The cross-over length is a function of the rupture width and is about 75 km for earthquakes with a saturated rupture width of 15 km. We compare our theoretical predictions with observed source parameters of some large strike-slip earthquakes, and they match up well. Our results also suggest that when large earthquakes have a fixed aspect ratio of rupture length to rupture width (which seems to be the case for most subduction earthquakes) the mean slip scales with the rupture dimension in the same way as small earthquakes. 相似文献
19.
In this study, we present a new and effective method to determine the dynamic source parameters (i.e., stress drop and strength distribution). We first assume that the kinematic source parameters, i.e., the slip and rupture time distributions on the fault plane, are known from the previous source inversion studies. Then, using the seismic source representation theorem we determine the dynamic stress field on a fault plane from known kinematic parameters. Finally, we determine the strength of the fault defined as the peak stress just before the rupture. We have tested the validity of this method by using an illustrative two-dimensional analytical example. To assess the applicability of this method, we have applied it to study the 1979 Imperial Valley earthquake, and obtained consistent results with those ofMiyatake's (1992) andQuin's (1990). Compared with previous methods, this new method is simple, straightforward and accurate, and needs much less calculation. Therefore, it is expected to be useful in exploring the seismic source process. 相似文献