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1.
封闭爆炸发生后常常产生大量的余震事件，本文对3次爆炸余震进行了分析和研究. 结果显示，余震波形持时很短, 70％以上的余震波形持时在2～7 s之间，持时频度衰减指数约为-1.6. 幂函数模型较好地描述了余震序列频度的整体变化特征, 爆炸后约两星期内，余震序列的频度衰减较快，衰减指数约为-1.0. 早期余震以群发式为主，后期余震以单发式为主. 对于同强度的爆炸, 因介质和地质构造的差异产生的余震数量相差几倍； 对于一次里氏震级为5.5级的爆炸，爆炸后约一个月内, 余震事件频度就接近了本底，此后仍有少量的余震发生. 相似文献
2.
An estimate of aftershock activity due to a theoretical underground nuclear explosion is produced using an aftershock rate model. The model is developed with data from the Nevada National Security Site, formerly known as the Nevada Test Site, and the Semipalatinsk Test Site, which we take to represent soft-rock and hard-rock testing environments, respectively. Estimates of expected magnitude and number of aftershocks are calculated using the models for different testing and inspection scenarios. These estimates can help inform the Seismic Aftershock Monitoring System (SAMS) deployment in a potential Comprehensive Test Ban Treaty On-Site Inspection (OSI), by giving the OSI team a probabilistic assessment of potential aftershocks in the Inspection Area (IA). The aftershock assessment, combined with an estimate of the background seismicity in the IA and an empirically derived map of threshold magnitude for the SAMS network, could aid the OSI team in reporting. We apply the hard-rock model to a M5 event and combine it with the very sensitive detection threshold for OSI sensors to show that tens of events per day are expected up to a month after an explosion measured several kilometers away. 相似文献
3.
通过海城地震余震活动序列资料，根据相空间中余震活动的演化特征，余震活动的功率谱和非线性地震活动演化方程的迭代解详细地研究了余震活动的基本特征．结果显示，余震活动除了通常熟悉的平均的衰减和周期性行为之外，还存在同样显著的混沌行为． 相似文献
4.
研究我国东部9次余震序列的总体特征得到:余震频度符合 n=n1t-h关系;频度和强度随时间衰减较慢;最大地震后3、4天内发生的余震所勾划的余震区常常比最终余震区小;多数余震分布在地壳中5至10公里的深度上.一些强余震前的中小余震时空分布有下述特征:（1）强余震前几天至十几天,余震序列的频度偏离正常衰减值;（2）强余震前有中小余震震中向下一次强余震的震中附近扩展或形成空区的现象;（3）强余震前震级序列出现缺震现象;（4）余震序列有准周期性.上述特性预示其后将发生强余震,同时表明强余震有类似于大地震的孕震过程.种种现象还表明余震序列在时间和空间上可能是由主震的直接余震和强余震的次级余震相互叠加所组成的.最后将某些特性和岩石试验结果进行了比较和讨论. 相似文献
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The current calibration function used in calculating the magnitude of natural earthquakes within 5km is a constant; a fact that causes several serious difficulties for the calculation of the magnitude of small and shallow-focus earthquakes. According to the attenuation law of explosions and the propagation theory of elastic waves, the calibration function is calculated for near field quakes from 0kin to 5kin. Magnitudes of two aftershock sequences are calculated. The magnitudes of most explosion earthquakes are small, ranging mainly from magnitude -0.5 to 1.0. The M-t chart of the explosive aftershocks is completely different from that of strong earthquake aftershocks. It not only shows positive columnar lines indieatJng large magnitudes but also short negative columnar lines indicating small magnitudes. 相似文献
6.
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
7.
采用双差定位方法,利用中国地震台网的数据对2017年8月9日精河6.6级地震的余震序列进行了重新定位。截至2017年8月14日16时,共获得209个余震的重新定位结果。结果显示,余震主要呈近EW向或NWW向分布,余震区长约50km,宽约17km。余震分布在主震的西侧,推断此次地震单侧破裂。余震震源深度为1～25km,其中,震级较大余震深度为8～17km。精河地震序列的余震活动随时间呈起伏状衰减,震后2天内比较活跃,此后出现较快衰减。随时间推移,余震区呈现中西部衰减慢、东部衰减快的特点。此次地震震中距2011年精河5.0级地震震中21km,相比2011年精河地震,其震源更深,震级更大,但震源机制解相近,均为逆冲型。结合区域构造背景分析认为,库松木契克山前断裂为此次地震发震构造的可能性较大。 相似文献
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本文利用CAP波形反演方法,获取了汶川MS8.0地震序列中312个具有较高信噪比波形资料的4级以上余震的震源机制解和震源深度. 基于震源深度空间分布与震源机制时空分布,分析了主震后余震区断层行为特征与应力场时空变化,并对龙门山断裂带中北段的发震断层面几何形态进行了初步探讨. 获得的主要认识如下:(1)余震震源深度分布存在显著的空间分段差异. 绵竹以西的余震区南段与平武以东的北段余震深度范围大于中段(绵竹-平武段),但深度小于5 km的5级以上超浅源地震主要分布在明显偏离龙门山断裂带走向的理县NW向分支与余震区北端NNE向分支,而中段余震主要分布在7~19 km深度. (2)余震机制类型存在明显的时空差异. 余震区中段逆冲型地震占绝对优势,理县NW向分支余震则以走滑型为主,机制类型随时间变化不显著. 沿龙门山断裂带走向的余震区南段,早期(2008年8月底前)逆冲型地震比例高于走滑型、晚期走滑型地震比例显著升高并超过逆冲型;而余震区北段早期走滑型地震占绝对优势、晚期逆冲型地震比例大幅上升且超过走滑型. 南、北两段余震机制类型比例的显著变化,可能是余震区两端断层调整性运动的表现. (3)节面走向及P轴方位优势方向均存在显著的空间差异. 南段NWW向P轴方位与区域应力场一致,中段及理县NW向分支P轴优势方向NEE,而北段具NWW和NEE两个优势方向,这种差异反映了余震活动除了受区域应力场控制外,还受到主震引发的局部应力场的控制. 节面走向的多方位分布则反映不同走向的构造参与了主震后的余震活动. (4)沿龙门山断裂带走向,余震区南段具深部缓倾角、浅部高倾角的铲形断面特征;中段深部倾角均值较稳定、浅部倾角均值随深度减小而增大;北段倾角均值相对稳定,显示其断面几何形态相对简单. 上述不同区段倾角均值随深度的变化揭示龙门山断裂带中北段断层面几何形态复杂. 相似文献
10.
Spatio-temporal characteristics of aftershocks and seismogenic structure of the 2011 MW9.0 Tohoku earthquake,Japan 
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下载免费PDF全文 The Tohoku megathrust earthquake, which occurred on March 11, 2011 and had an epicenter that was 70 km east of Tohoku, Japan, resulted in an estimated ten's of billions of dollars in damage and a death toll of more than 15 thousand lives, yet few studies have documented key spatio-temporal seismogenic characteristics. Specifically, the temporal decay of aftershock activity, the number of strong aftershocks (with magnitudes greater than or equal to 7.0), the magnitude of the greatest aftershock, and area of possible aftershocks. Forecasted results from this study are based on Gutenberg-Richter's relation, Bath's law, Omori's law, and Well's relation of rupture scale utilizing the magnitude and statistical parameters of earthquakes in USA and China (Landers, Northridge, Hector Mine, San Simeon and Wenchuan earthquakes). The number of strong aftershocks, the parameters of Gutenberg-Richter's relation, and the modified form of Omori's law are confirmed based on the aftershock sequence data from the MW9.0 Tohoku earthquake. Moreover, for a large earthquake, the seismogenic structure could be a fault, a fault system, or an intersection of several faults. The seismogenic structure of the earthquake suggests that the event occurred on a thrust fault near the Japan trench within the overriding plate that subsequently triggered three or more active faults producing large aftershocks. 相似文献
11.
在地震序列的早期阶段获得科学可靠的余震预测结果,始终是地震预测研究的前沿课题.针对新近发展的Omi-R-J方法的适用性问题,以及相比于传统的Reseanberg-Jones （R-J）模型在地震序列参数拟合、余震预测效能上的差异等问题,本文以2017年四川九寨沟MS7.0地震序列为例,利用多时间窗的连续滑动拟合、预测和检验,以及通过构建重采样随机地震序列目录的系统检验等方式,开展了应用研究和比较研究.结果表明：相比于R-J模型,Omi-R-J方法可在余震记录较不完整的地震序列早期阶段获得稳定、可靠的序列参数,p值、c值和b值的标准差相比于R-J模型参数明显减小.N-test方法检验结果表明,在R-J模型等传统方法无法获得预测结果的地震序列早期阶段,Omi-R-J方法预测结果可以较高的比例通过N-test检验,在后续时段的预测效果也明显优于R-J模型.利用随机地震序列目录的测试结果表明,余震记录完整性下降对Omi-R-J方法预测结果的影响相对较小,在全部时段的完整性下降的影响高于在部分时段的完整性下降.上述结果对进一步地将Omi-R-J方法应用在震后早期余震预测中具有一定科学借鉴意义. 相似文献
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Long aftershock sequences in North China and Central US: implications for hazard assessment in mid-continents 下载免费PDF全文
下载免费PDF全文 Because seismic activity within mid-continents is usually much lower than that along plate boundary zones, even small earthquakes can cause widespread concerns, especially when these events occur in the source regions of previous large earthquakes. However, these small earthquakes may be just aftershocks that continue for decades or even longer. The recent seismicity in the Tangshan region in North China is likely aftershocks of the 1976 Great Tangshan earthquake. The current earthquake sequence in the New Madrid seismic zone in central United States, which includes a cluster of M ~ 7.0 events in 1811–1812 and a number of similar events in the past millennium, is believed to result from recent fault reactivation that releases pre-stored strain energy in the crust. If so, this earthquake sequence is similar to aftershocks in that the rates of energy release should decay with time and the sequence of earthquakes will eventually end. We use simple physical analysis and numerical simulations to show that the current sequence of large earthquakes in the New Madrid fault zone is likely ending or has ended. Recognizing that mid-continental earthquakes have long aftershock sequences and complex spatiotemporal occurrences are critical to improve hazard assessments. 相似文献
13.
较大的余震可能造成额外损失并有二次触发建筑物受灾的风险。为研究余震序列衰减规律,文章尝试采用指数衰减模型拟合分析5个不同地区余震序列,并借助修正赤池信息准则、贝叶斯信息准则与调整后R2,分析其与传统余震衰减模型的性能。结果表明,指数模型描述余震序列衰减规律的能力与修正的大森余震模型、修正的拉伸指数模型接近。尤其对于四川长宁MS6.0余震序列和云南彝良MS5.7余震序列,指数模型表现优于其他两种模型。指数模型参数具有明确的物理意义：参数A与r之和能够准确代表强震后的实际初始余震数,5个余震序列初始余震数偏差均小于1.70%;参数k可作为反映余震序列衰减快慢的特征值,k值越大则余震序列衰减越慢,其值与主震震级呈反比例关系。 相似文献
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The aftershock activity of the May 12, 2008 Wenchuan Ms8.0 Earthquake Sequence shows an obvious segmented feature. Most of the large aftershocks were distributed in the north and south parts of the aftershock zone. Thrusting was dominant with a small amount of strike-slip component in the south part. The aftershock activity decayed gradually, presenting the sequence features of a mainshock-aftershock pattern. The north part was the ending area of the maiushock fracture where strike-slipping was dominant, showing an obvious swarm feature. Therefore it became the major area for large aftershocks. The modulation of the earth tide on aftershock activity is remarkable; most large aftershocks occur during the period of flood and neap tide. The time period around 16:00 was the dominant occurring time for large aftershocks. The p-value, a parameter of modified Omori formula, increases gradually with time, and reaches about 1 at the end. Based on previous study, the sequence patterns, magnitude of maximum aftershock, as well as the duration of aftershock activity has been discussed. The primary results also show that the magnitude difference between the maiushockand the maximum aftershock is proportional to the rupture size of the maiushock for huge earthquakes of about Ms8.0. This means that when the magnitudes of the earthquakes are nearly the same, large rupture size corresponds to sufficient energy release. 相似文献
15.
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
16.
IntroductionThesouthernpartofKhorasanProvinceineast-centralIranisoneoftheseismicallyactiveregionsintheMiddleeast.Historicalreportsindicatedseveralearthquakeshavecausedseveredestructionsandhumanlossinthisregionduringthepastcenturies(Ambraseys,Melville,1982).Theinstrumentallyrecordedearthquakesaswellastheexistenceofseveralactivefaultsalsosug-gestedthattheregionhadahighpotentialofseismicactivities.OnMay10,1997at07:57:29.6GMT,12:27:29.6localtime,ashallowdestructiveearthquakewithoutanyfeltfores… 相似文献
17.
We obtained a catalog of early aftershocks of the 2013 Lushan earthquake by examining waveform from a nearby station MDS which is 30.2 km far away from the epicenter, and then we analyzed the relation between aftershock rate and time. We used time-window ratio method to identify aftershocks from continuous waveform data and compare the result with the catalog provided by China Earthquake Networks Center (CENC). As expected, a significant amount of earthquakes is missing in CENC catalog in the 24 h after the main shock. Moreover, we observed a steady seismicity rate of aftershocks nearly in the first 10,000 s before an obvious power-law decay of aftershock activity. We consider this distinct early stage which does not fit the Omori law with a constant p (p ~ 1) value as early aftershock deficiency (EAD), as proposed by previous studies. Our study suggests that the main shock rupture process is different from aftershocks’ processes, and EAD can vary in different cases as compared to earthquakes of strike-slip mechanism in California. 相似文献
18.
选取了汶川地震主震后的2008年5月12日——2009年8月31日, 震级为3.0le;MSle;5.0的余震4240次．利用波形互相关方法得到其P波到时,用双差定位方法对其进行定位,最终得到了2441次重新定位的结果．统计定位误差（两倍标准偏差）在E-W方向为0.4 km,N-S方向为0.4 km,垂直方向为0.7 km．定位结果表明,汶川地震的余震深度集中在10——20 km,震中分布与龙门山中央断裂带的走向关系密切．沿龙门山断裂的地震分布具有明显的分段性,西南段呈水平带状分布,东北段接近垂直分布,且在北川附近存在深度突变．这与龙门山断裂的地震在西南段多表现为逆冲,东北段多表现为走滑的现象相吻合．在深度剖面上地震的空间分布存在分立的特征,通过对比前人在此地区浅层的地震剖面资料, 发现地震空间分布与已探知的浅部断层有较好的对应关系． 相似文献
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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
20.
大森-宇津定律的一种可能机制以唐山大地震为例 总被引：2，自引：0，他引：2
为了探讨大森-宇津定律的物理机制, 本文在余震区等效黏度远低于其外部, 且构造应力场在整个余震活动时间间隔内基本保持不变的假设条件下, 提出了一个开尔文黏弹性地震震源体概念模型． 该模型可用于模拟主震后断层蠕变和震源区应力调整触发的余震序列以及蠕变停止后余震终结、 介质恢复到弹性状态、 断层重新闭锁和积累下一次地震的整个过程． 有限元方法可用来计算非均匀黏弹性地震震源体模型中主震和每次余震所引起的应力场及其随时间的演化过程． 在此基础上, 采用开尔文黏弹性地震震源体概念模型和有限元方法模拟了1976年唐山MS7.8地震余震序列． 结果表明: 经验的大森-宇津定律可以用开尔文黏弹性震源体模型来解释, 这意味着余震衰减的频度取决于蠕变的速率; 余震序列持续时间受控于震源体的黏度, 即黏度越大, 蠕变时间越长, 余震持续的时间也就越长． 相似文献