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1.
Earthquakes are generally clustered, both in time and space. Conventionally, each cluster is made of foreshocks, the mainshock, and aftershocks. Seismic damage can possibly accumulate because of the effects of multiple earthquakes in one cluster and/or because the structure is unrepaired between different clusters. Typically, the performance-based earthquake engineering (PBEE) framework neglects seismic damage accumulation. This is because (i) probabilistic seismic hazard analysis (PSHA) only refers to mainshocks and (ii) classical fragility curves represent the failure probability in one event, of given intensity, only. However, for life cycle assessment, it can be necessary to account for the build-up of seismic losses because of damage in multiple events. It has been already demonstrated that a Markovian model (i.e., a Markov chain), accounting for damage accumulation in multiple mainshocks, can be calibrated by maintaining PSHA from the classical PBEE framework and replacing structural fragility with a set of state-dependent fragility curves. In fact, the Markov chain also works when damage accumulates in multiple aftershocks from a single mainshock of known magnitude and location, if aftershock PSHA replaces classical PSHA. Herein, this model is extended further, developing a Markovian model that accounts, at the same time, for damage accumulation: (i) within any mainshock–aftershock seismic sequence and (ii) among multiple sequences. The model is illustrated through applications to a series of six-story reinforced concrete moment-resisting frame buildings designed for three sites with different seismic hazard levels in Italy. The time-variant reliability assessment results are compared with the classical PBEE approach and the accumulation model that only considers mainshocks, so as to address the relevance of aftershocks for life cycle assessment. 相似文献
2.
依据1970年以来记录相对完整的294次50级以上地震序列资料，研究中国大陆中强地震余震序列统计特征，探讨序列类型、最大余震震级、强余震活动持续时间等与主震震级及主震断层性质之间的关系.中国大陆孤立型、主余型及多震型地震余震序列分别约占23%、59%及18%.其中走滑型、具有倾滑分量的走滑型、具有走滑分量的倾滑型及逆冲型分别占48%、24%、17%及11%. 余震序列1年内最大余震震级与主震震级正相关，但主震震级较低时相对离散，孤立型序列离散程度较高，主余型及多震型序列线性相关性较好.绝大多数序列最大余震均发生在震后200天内，少数具有晚期强余震的序列主要属主余型序列,孤立型及多震型序列通常没有晚期强余震发生.68%的序列1年内最大余震发生在震后10天内，77%发生在震后30天之内,95%发生在震后120天之内.序列最大余震发生时间及5、6级强余震活动持续时间与序列类型及主震震级大小有关，多震型序列最大余震发生最快，孤立型次之、主余型最长.若仅就主余型序列而言，当主震震级较高时最大余震与主震间时间间隔相对较短，主震震级较低时最大余震与主震间时间间隔相对较长. 相似文献
3.
本文介绍了余震危险性概率分析的概念，完整列出其相关公式的解析表达式并阐述了余震危险性概率分析的具体方法。以2017年九寨沟MS7.0地震为例，首先，求得该地震余震序列的相关参数，结果显示:九寨沟MS7.0地震余震序列理论最大余震震级约为ML5.3；b值约为0.784 1，明显低于中国西南地区同类型的其它地震，表明九寨沟地震余震区应力水平相对较高；p值约为1.109 7，明显高于中国西南地区同类型的其它地震，表明九寨沟地震余震序列随时间衰减较快。其次，计算此次地震余震与主震释放能量的比例关系，结果显示:在九寨沟MS7.0地震事件中，截止到10月22日约99.69%的能量为主震所释放，0.31%的能量为余震所释放。最后，利用九寨沟MS7.0余震序列参数结果并结合衰减关系，分别计算了主震后0—1天、1—10天、10—30天和90—100天内不同断层距内不同水平的峰值加速度和峰值速度的超越概率，结果显示:随着断层距增加，在相同时间间隔内超越概率的值呈下降趋势；在震后第一天内余震危险性最高，随着震后时间增加，相应的超越概率值呈现出明显下降趋势，表明九寨沟MS7.0地震余震危险性主要来自早期余震。本文的相关成果可以为震后地震危险性分析提供参考，并为短时间内应急救援及灾后重建提供辅助决策意见。 相似文献
4.
针对九寨沟MS7.0地震之后不同时间段的余震序列目录，利用推定最大余震震级，给出了实际最大余震震级的估计值。结果表明，推定最大余震震级随主震后时间尺度的延长而趋于稳定，且该值与实际发生的最大余震的震级一致。需要强调的是，就九寨沟地震序列而言，当余震数据较为完备时，采用主震后较短时间段内（1～2天）的余震目录就可以较准确地估算出主震区域内可能发生的最大余震震级。实际上，主震后12h（0.5天）的余震数据已完全可以给出最大余震震级的有效下限。此外，计算中我们采用了里氏震级ML和面波震级MS的余震目录，结果显示，2种震级类型目录的估算结果完全一致，表明利用推定最大余震震级估算实际最大余震震级的方法不受震级类型的影响。据此，该最大余震震级快速评估方法可进一步推广应用于我国大陆地区中强震后强余震灾害分析评估中。目前的拟合技术也显示出随着测震技术的不断进步以及余震识别能力的提高，快速评估方法可以在主震后短时间（<1天）内准确地预测可能发生的最大余震震级。 相似文献
5.
A large mainshock may trigger numerous aftershocks within a short period, and nuclear power plant (NPP) structures have the probability to be exposed to mainshock–aftershock seismic sequences. However, the researchers focused on seismic analyses of reinforced concrete containment (RCC) buildings under only mainshocks. The aim of this paper is to thoroughly investigate the dynamic responses of a RCC building under mainshock–aftershock seismic sequences. For that purpose, 10 as-recorded mainshock–aftershock seismic sequences with two horizontal components are considered in this study, and a typical three-dimensional RCC model subjected to the selected as-recorded seismic sequences is established. Peak ground accelerations (PGAs) of mainshocks equal to 0.3 g (safe shutdown earthquake load-SSE load) are considered in this paper. The results indicate that aftershocks have a significant effect on the responses of the RCC in terms of maximum top accelerations, maximum top displacements and accumulated damage. Furthermore, in order to preserve the RCC from large damage under repeated earthquakes, local damage and global damage indices are suggested as limitations under only mainshocks. 相似文献
6.
Aftershocks have been shown to exacerbate earthquake‐induced financial losses by causing further damage to structural and nonstructural components in buildings that have already been affected by a mainshock event and increasing the duration of disrupted functionality. Whereas seismic loss assessment under isolated events has been addressed thoroughly in previous studies, comparatively less has been accomplished in the area of loss assessment under sequences of mainshock‐aftershock ground motions. The main objective of the current study is to formulate a comprehensive framework for quantifying financial losses under sequential seismic events. The proposed framework is capable of accounting for the uncertainties in the state of structure due to accumulation of earthquake‐induced damage, the time‐dependent nature of seismic hazard in the post‐mainshock environment, and the uncertainties in the occurrence of mainshock and aftershock events. Application of the proposed framework to a 4‐story reinforced concrete moment frame shows that consideration of aftershocks could increase lifecycle earthquake‐induced losses by up to 30% compared with mainshock‐only assessments. 相似文献
7.
Megathrust earthquake sequences, comprising mainshocks and triggered aftershocks along the subduction interface and in the overriding crust, can impact multiple buildings and infrastructure in a city. The time between the mainshocks and aftershocks usually is too short to retrofit the structures; therefore, moderate‐size aftershocks can cause additional damage. To have a better understanding of the impact of aftershocks on city‐wide seismic risk assessment, a new simulation framework of spatiotemporal seismic hazard and risk assessment of future M9.0 sequences in the Cascadia subduction zone is developed. The simulation framework consists of an epidemic‐type aftershock sequence (ETAS) model, ground‐motion model, and state‐dependent seismic fragility model. The spatiotemporal ETAS model is modified to characterise aftershocks of large and anisotropic M9.0 mainshock ruptures. To account for damage accumulation of wood‐frame houses due to aftershocks in Victoria, British Columbia, Canada, state‐dependent fragility curves are implemented. The new simulation framework can be used for quasi‐real‐time aftershock hazard and risk assessments and city‐wide post‐event risk management. 相似文献
8.
破坏性地震强度预测可用于工程领域抗震设防以及地震危险性分析评估，是防震减灾中一项很重要的基础工作.为了再现九寨沟地震的地震动强度，评估缺失强震记录的九寨章扎台站的地震动强度，本文用经验格林函数法对九寨沟地震进行了数值模拟.选取了震源周边地震动峰值加速度超过10 Gal的10个强震台站进行模拟.因未得到九寨沟地震的余震，初次尝试将汶川地震和定西地震的余震作为格林函数模拟九寨沟地震.模拟结果整体上可以反映各台站地震动的强度特征，尤其是地震动高频成份拟合较好.模拟值的地震动峰值加速度、时程数据、反应谱等与观测值拟合较好.预测结果显示漳扎镇的地震动峰值加速度值约为180~200 Gal.预测结果也表明在缺少大震的余震记录时，经验格林函数法使用其他大震的余震同样可以再现目标地震的强度特征.本研究也为经验格林函数方法在缺乏小震记录地区的使用积累了经验.最后总结了格林函数的选取标准，为经验格林函数方法来预测未来强震动特征积累了经验. 相似文献
9.
2017年8月8日在青藏高原东缘四川省九寨沟县发生M7.0级强烈地震，极震区烈度达Ⅸ度，但无明显地表破裂，一定程度上限制了发震构造的确定和后续地震危险性判定.本文基于截止至2017年8月14日的地震资料，采用多阶段定位方法，对主震及余震进行了重新定位，同时，利用CAP波形反演方法，获得了M7.0主震与13次ML ≥ 4.0级余震的震源机制解和震源矩心深度，进而初步分析了本次地震的发震构造.结果显示，九寨沟M7.0地震的矩震级MW6.4，震源矩心深度5 km，表明主震发生在上地壳浅部，与2003年伊朗巴姆（Bam）MW6.5地震特征极为相似；12次ML ≥ 4.0级余震的震源矩心深度6~12 km，显示这些余震发生在主震下部，仅1次例外.重新定位后的余震震中呈NW-SE向窄带展布，位于近NS向的岷江断裂与近EW向的东昆仑断裂带东端分支塔藏断裂所夹持的区域，余震带长轴长约38 km，主震位于余震带中部.根据余震震中分布、主震及余震震源机制解等，推测本次九寨沟M7.0地震及其余震的主发震构造为位于岷江断裂与塔藏断裂之间的树正断裂.震源机制解揭示，树正断裂呈左旋走滑，走向约152°，近SE，倾向SW，倾角约70°，该断裂应属于东昆仑断裂东端的分支断裂之一，或与东南侧的虎牙断裂构成统一断裂系. 相似文献
10.
对大地震发生后强余震的震源机制,基于主要地震断层上小余震的时空分布进行了详细研究.近期在中国境内发生的强烈板内地震,如1976年唐山、1975年海城、1976年盐源——宁蒗等地震曾被中国地震台网很好记录.主震刚发生后的小余震以及强余震前后的小余震的震源用 S——P 时间的收敛法进行测定.强余震的断层是依靠这些小余震的震中分布来描绘的.可以看出有三种情况.第一,在主震断层区内,一次强余震发生在较小余震的比较不密集的部位;第二,一次强余震沿断层发生并与主震断层是共轭的;第三,一次强余震在沿平行并离开主震断层的断层上发生.可以认为,地质条件控制着强余震的发生.作为强余震的可能前兆,则有唐山地震的一次强余震,震级为7.1.其发生前,出现一些前震以及在接近主震断层方向上的某些地震台所记录的初动方向有变化.可以设想,这里的应力场在强余震发生前是有所变化的. 相似文献
11.
2008年"5·12"汶川特大地震发生后，固定及流动台站获得了数量可观的余震地震动数据，为地震危险性分析和地震动衰减规律研究提供了丰富的数据。通过Gutenberg-Richter关系分析得到汶川地震余震震级-频度分布（FMD），结合Båth定律预估得到逼近实际的最大预估余震震级，基于修正的Omori定律拟合得到余震发生率与主震后时间的关系。主余震统计特性显示Ms4.0~6.4范围内的余震记录震中距及震级分布相对均匀，可作为建立地震动衰减规律的依据。故针对土层地表及基岩地表分别进行了EW、NS和UD三个方向的统计回归分析，给出了2种地表情况下三向地震动峰值加速度的定量衰减关系表达式。 相似文献
12.
《地震研究进展（英文）》2023,3(1):100184
The 2022 MS 6.8 Luding earthquake is the strongest earthquake in Sichuan Province, Western China, since the 2017 MS 7.0 Jiuzhaigou earthquake. It occurred on the Moxi fault in the southeastern segment of the Xianshuihe fault, a tectonically active and mountainous region with severe secondary earthquake disasters. To better understand the seismogenic mechanism and provide scientific support for future hazard mitigation, we summarize the preliminary results of the Luding earthquake, including seismotectonic background, seismicity and mainshock source characteristics and aftershock properties, and direct and secondary damage associated with the mainshock. The peak ground displacements in the NS and EW directions observed by the nearest GNSS station SCCM are ～35 mm and ～55 mm, respectively, resulting in the maximum coseismic dislocation of 20 mm along the NWW direction, which is consistent with the sinistral slip on the Xianshuihe fault. Back-projection of teleseismic P waves suggest that the mainshock rupture propagated toward south-southeast. The seismic intensity of the mainshock estimated from the back-projection results indicates a Mercalli scale of VIII or above near the ruptured area, consistent with the results from instrumental measurements and field surveys. Numerous aftershocks were reported, with the largest being MS 4.5. Aftershock locations (up to September 18, 2022) exhibit 3 clusters spanning an area of 100 km long and 30 km wide. The magnitude and rate of aftershocks decreased as expected, and the depths became shallower with time. The mainshock and two aftershocks show left-lateral strike-slip focal mechanisms. For the aftershock sequence, the b-value from the Gutenberg-Richter frequency-magnitude relationship, h-value, and p-value for Omori’s law for aftershock decay are 0.81, 1.4, and 1.21, respectively, indicating that this is a typical mainshock-aftershock sequence. The low b-value implies high background stress in the hypocenter region. Analysis from remote sensing satellite images and UAV data shows that the distribution of earthquake-triggered landslides was consistent with the aftershock area. Numerous small-size landslides with limited volumes were revealed, which damaged or buried the roads and severely hindered the rescue process. 相似文献
13.
1978年5月18日海城地震(Ms=6.0)发生在1975年2月4日海城破坏性地震(Ms=7.3)余震区的空区内.1975年2月4日海城7.3级强震发生之后,其余震(Ms2.0)的月频度衰减异常缓慢(P=0.73),而6级地震发生之后 P 值明显增大,即6级地震发生在月频度衰减曲线的拐点上.这次6级地震之前不同于7.3级强震前,在震源区没有丰富的前震活动.6级地震是7.3级强震的最大余震,作者认为它是区域应力在未曾充分破裂的空区内再次集中积累而发生的余震. 相似文献
14.
According to the current seismic codes, structures are designed to resist the first damaging earthquake during their service life. However, after a strong main shock, a structure may still face damaging aftershocks. The main shock‐aftershock sequence may result in major damage and eventually the collapse of a structure. Current studies on seismic hazard mainly focus on the modeling and simulation of main shocks. This paper proposes a 3‐step procedure to generate main shock‐aftershock sequences of pairs of horizontal components of a ground motion at a site of interest. The first step generates ground motions for the main shock using either a source‐based or site‐based model. The second step generates sequences of aftershocks' magnitudes, locations, and times of occurrence using either a fault‐based or seismicity‐based model. The third step simulates pairs of ground motion components using a new empirical model proposed in this paper. We develop prediction equations for the controlling parameters of a ground motion model, where the predictors are the site condition and the aftershock characteristics from the second step. The coefficients in the prediction equations and the correlation between the model parameters (of the 2 horizontal components of 1 record and of several records in 1 sequence) are estimated using a database of aftershock accelerograms. A backward stepwise deletion method is used to simplify the initial candidate prediction equations and avoid overfitting the data. The procedure, based on easily identifiable engineering parameters, is a useful tool to incorporate effects of aftershocks into seismic analysis and design. 相似文献
15.
本文采用离散波数法,计算了2014年于田MS7.3地震的断层破裂在近场和远场产生的库仑破裂应力变化,并结合地震活动特征,讨论了MS7.3地震对后续余震活动和远场区域小震活动的动态应力触发作用.结果表明, ① MS7.3地震产生的库仑破裂应力变化对其西南侧主体余震区的地震活动起到了抑制作用,这可能是本次MS7.3地震序列余震活动水平不高的主要原因;距主震约30 km的北东方向余震区后续地震活动受到了主震产生的动态和静态应力变化的共同触发作用,动态应力变化峰值为2.78 MPa,静态应力变化为0.80 MPa,这与该区余震较为活跃相一致;距主震约45 km的北部余震区受到动态应力触发作用,应力变化峰值为0.72 MPa. ② MS7.3地震产生的动态库仑应力变化空间分布呈非对称性,其中北东方向、北部余震分布与动态应力变化正值区存在相关性,从应力变化的角度解释了MS7.3地震的后续余震空间活动特征. ③ MS7.3地震在沙雅、伽师地区的远场接收点产生的动态应力变化峰值分别为0.09 MPa、0.1 MPa,对两个区域的小震活动具有动态触发作用. 相似文献
16.
2010年9月3日16时35分46秒新西兰南岛Greendale附近发生了MW7.0地震, 震源深度约10.0 km. 2011年2月21日新西兰南岛又发生了MW6.1地震, 为2010年MW7.0主震后最大的一次余震, 震源深度约5.0 km, 发震断层为Christchurch南约9 km一条近东西走向逆冲的隐伏断层, 该地震造成Christchurch城内多处建筑物严重损毁. 本文分析了2010年新西兰地震事件MW7.0主震与MW6.1余震强地面运动的特征. 新西兰MW6.1余震近场强地面运动整体高于MW7.0主震. 将主震和余震的强震观测记录分别与新一代衰减关系(NGA)进行对比, 发现余震强震观测数据整体高于其震级对应的NGA. 分别选取距离主震和余震震中最近且强震观测记录最高的两个台站(GDLC台站和HVSC台站)作为参照台站, 建立动态复合震源模型(DCSM)及有限断层随机振动模型(SFFM)进行强地面运动的模拟计算, 分析两种模型的模拟结果并对比二者的优势及局限, 以便在未来工作中更好地通过模型计算强地面运动特征, 实现区域化特征快速、 实时分析及局部重点、 细致分析相结合的目标. 相似文献
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Egill Hauksson Joann Stock Kate Hutton Wenzheng Yang J. Antonio Vidal-Villegas Hiroo Kanamori 《Pure and Applied Geophysics》2011,168(8-9):1255-1277
The El Mayor-Cucapah earthquake sequence started with a few foreshocks in March 2010, and a second sequence of 15 foreshocks of M?>?2 (up to M4.4) that occurred during the 24?h preceding the mainshock. The foreshocks occurred along a north?Csouth trend near the mainshock epicenter. The M w 7.2 mainshock on April 4 exhibited complex faulting, possibly starting with a ~M6 normal faulting event, followed ~15?s later by the main event, which included simultaneous normal and right-lateral strike-slip faulting. The aftershock zone extends for 120?km from the south end of the Elsinore fault zone north of the US?CMexico border almost to the northern tip of the Gulf of California. The waveform-relocated aftershocks form two abutting clusters, each about 50?km long, as well as a 10?km north?Csouth aftershock zone just north of the epicenter of the mainshock. Even though the Baja California data are included, the magnitude of completeness and the hypocentral errors increase gradually with distance south of the international border. The spatial distribution of large aftershocks is asymmetric with five M5+ aftershocks located to the south of the mainshock, and only one M5.7 aftershock, but numerous smaller aftershocks to the north. Further, the northwest aftershock cluster exhibits complex faulting on both northwest and northeast planes. Thus, the aftershocks also express a complex pattern of stress release along strike. The overall rate of decay of the aftershocks is similar to the rate of decay of a generic California aftershock sequence. In addition, some triggered seismicity was recorded along the Elsinore and San Jacinto faults to the north, but significant northward migration of aftershocks has not occurred. The synthesis of the El Mayor-Cucapah sequence reveals transtensional regional tectonics, including the westward growth of the Mexicali Valley and the transfer of Pacific?CNorth America plate motion from the Gulf of California in the south into the southernmost San Andreas fault system to the north. We propose that the location of the 2010 El Mayor-Cucapah, as well as the 1992 Landers and 1999 Hector Mine earthquakes, may have been controlled by the bends in the plate boundary. 相似文献
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Data replenishment of five moderate earthquake sequences in Japan,with semi-automatic cluster selection 
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下载免费PDF全文 Missing early aftershocks following relatively large or moderate earthquakes can cause significant bias in the analysis of seismic catalogs. In this paper, we systematically address the aftershock missing problem for five earthquake sequences associated with moderate-size events that occurred inland Japan, by using a stochastic replenishing method. The method is based on the notion that if a point process (e.g., earthquake sequence) with time-independent marks (e.g., magnitudes) is completely observed, it can be transformed into a homogeneous Poisson process by a bi-scale empirical transformation. We use the Japan Meteorological Agency (JMA) earthquake catalog to select the aftershock data and replenish the missing early events using the later complete part of each aftershock sequence. The time windows for each sequence span from 6 months before the mainshock to three months after. The semi-automatic spatial selection uses a clustering method for the epicentral selection of earthquakes. The results obtained for the original JMA catalog and replenished datasets are compared to get insight into the biases that the missing early aftershocks may cause on the Omori-Utsu law parameters’ estimation, characterizing the aftershock decay with time from the mainshock. We have also compared the Omori-Utsu law parameter estimates for two datasets following the same mainshock; the first dataset is the replenished sequence, while the second dataset has been obtained by waveform-based analysis to detect early aftershocks that are not recorded in the JMA catalog. Our results demonstrate that the Omori-Utsu law parameters estimated for the replenished datasets are robust with respect to the threshold magnitude used for the analyzed datasets. Even when using aftershock time windows as short as three days, the replenished datasets provide stable Omori-Utsu law parameter estimations. The p-values for all the analyzed sequences are about 1.1 and c-values are significantly smaller compared to those of original datasets. Our findings prove that the replenishment method is a fast, reliable approach to address the missing aftershock problem. 相似文献
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本文针对2008年5月12日四川汶川MW7.9地震后的余震目录，采用2004年Shcherbakov和Turcotte提出的最大余震震级推断法，给出了最大余震震级的估计值。结果表明，采用现有的余震数据，在大震级区间可能存在一定数量的余震缺失，这造成了余震数据与Gutenberg-Richter定律曲线在大震级区间的差异，导致推断的最大余震震级与使用目录中的最大余震震级存在明显差异。利用震级与断层长度或地表破裂长度之间的经验关系可以看出，由灌县—江油断裂的破裂尺度得到的震级与推断最大余震震级基本一致。根据前人给出的断层摩擦失稳时间模型和Brune近断层质点运动模型，本文进一步探讨了汶川地震北川—映秀断裂对灌县—江油断裂的触发作用，认为北川—映秀断裂破裂所辐射出的S波可以在短时间内使得灌县—江油断裂发生失稳，进而产生宏观破裂并形成地震，因此由灌县—江油断裂破裂形成的地震可能为汶川地震的最大余震。 相似文献