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1.
《地震研究进展（英文）》2021,1(1):100002
An improved understanding of postseismic crustal deformation following large subduction earthquakes may help to better understand the rheological properties of upper mantle and the slip behavior of subduction interface. Here we construct a three-dimensional viscoelastic finite element model to study the postseismic deformation of the 2014 MW8.1 Iquique, Chile earthquake. Elastic units in the model include the subducting slab, continental and oceanic lithospheres. Rheological units include the mantle wedge, the oceanic asthenosphere and upper mantle. We use a 2 km thick weak shear zone attached to the subduction fault to simulate the time-dependent stress-driven afterslip. The viscoelastic relaxation in the rheological units is represented by the Burgers rheology. We carry out grid-searches on the shear zone viscosity, thickness and viscosity of the asthenosphere, and they are determined to be 1017 Pa s, 110 km and 2 × 1018 Pa s, respectively. The stress-driven afterlsip within the first two years is up to ~47 cm and becomes negligible after two years (no more than 5 cm/yr). Our results suggest that a thin, low-viscosity oceanic asthenosphere together with a weak shear zone attached to the fault are required to better reproduce the observed postseismic deformation. 相似文献
2.
Kuo-En Ching Kaj M. Johnson Ruey-Juin Rau Ray Y. Chuang Long-Chen Kuo Pei-Ling Leu 《Earth and Planetary Science Letters》2011,301(1-2):78-86
We invert measurements of coseismic displacements from 139 continuously recorded GPS sites from the 2010, Jiashian, Taiwan earthquake to solve for fault geometry and slip distribution using an elastic uniform stress drop inversion. The earthquake occurred at a depth of ~ 23 km in an area between the Western Foothills fold-and-thrust belt and the crystalline high mountains of the Central Range, providing an opportunity to examine the deep fault structure under Taiwan. The inferred rupture plane is oblique to the prominent orientation of thrust faults and parallel to several previously recognized NW-striking transfer zones that appear to connect stepping thrusts. We find that a fault striking 318°–344° with dip of 26°–41° fits the observations well with oblique reverse-sinistral slip under a low stress drop of about 0.5 MPa. The derived geodetic moment of 2.92 × 1018 N-m is equivalent to a Mw = 6.24 earthquake. Coseismic slip is largely concentrated within a circular patch with a 10-km radius at the depth between 10 and 24 km and maximum slip of 190 mm. We suggest this earthquake ruptured the NW-striking Chishan transfer fault zone, which we interpret as a listric NE-dipping lateral ramp with oblique slip connecting stepping thrust faults (ramps). The inferred slip on the lateral ramp is considerably deeper than the 7–15 km deep detachment identified in previous studies of western Taiwan. We infer an active basal detachment under western Taiwan at a depth of at least ~ 20–23 km based on these inversion results. The earthquake may have nucleated at the base of the lateral ramp near the intersection with the basal detachment. Coulomb stress change calculations suggest that this earthquake moved several NE-striking active thrust faults in western Taiwan nearer to failure. 相似文献
3.
基于InSAR技术,利用欧空局升降轨Sentinel-1A/IW宽幅数据,获取了2017年8月8日四川九寨沟7.0级地震InSAR同震形变场,并以升降轨InSAR观测结果为约束,反演了断层滑动分布,基于三种不同接收断层计算了同震库仑应力变化.结果表明,同震形变场发生在塔藏断裂、岷江断裂和虎牙断裂交汇的三角地带,升降轨干涉位移均显示本次地震的形变场影响范围约为50 km×50 km,形变场长轴方向为NW向,升降轨观测的形变量相反,反映断层运动性质以走滑运动为主,升降轨数据观测得到的最大LOS （Line of Sight,视线向）形变量分别为~22 cm和~14 cm.非对称形变场反映出断层两侧的运动差异.反演结果显示,最大滑动量约为1 m,平均滑动角为-9°,矩震级为MW6.5,地震破裂主要集中在地下1~15 km深度范围内,但整体而言本次地震破裂较为充分,基本将该区域1973年及1976年4次 > MW6.0地震的破裂空区完全破裂.考虑到塔藏断裂和虎牙断裂的运动性质,可初步判定发震断层为虎牙断裂北侧延伸分支.基于三种不同接收断层模型的同震库仑应力变化计算结果反映出该区域以应力释放为主,进一步触发较大走滑型余震的可能性不大. 相似文献
4.
《地震研究进展（英文）》2021,1(4):100065
The focal mechanism solution of the Shiqu MS 4.4 earthquake occurred on May 16th, 2017 in Sichuan Province is studied by the gCAP method using the waveform data from the regional seismic networks in Sichuan, Qinghai, Tibet and Gansu provinces. The strike/dip/dipping angle of the first nodal plane are 214°/80°/167° and those of the second nodal plane are 306°/77°/10°, the optimal centroid depth is 7.3 ± 0.6 km and the moment magnitude is MW 4.5. Furthermore, the study investigates the robustness of the results against the error of crustal velocity structure, location, data quality and difference of seismic parameters, subsequently obtaining a stable resolved focal mechanism. According to the geological structure in the seismogenic area, spatial distribution of aftershock sequenceof the regional tectonic stress field, and the focal mechanism of the main shock, we suggest that the Shiqu earthquake is induced by a left-lateral strike-slip mechanism and the second nodal plane is inferred to be the seismogenic fault, consistent with the geometry of the Changshagongma fault which is the secondary fault of the northwest part of the Xianshuihe fault zone. 相似文献
5.
Samar Amini Roland Roberts Mohammad Raeesi Zaher Hossein Shomali Bjorn Lund Zoya Zarifi 《Journal of Seismology》2018,22(4):815-831
An intraplate earthquake doublet, with 11-min delay between the events, devastated the city of Varzeghan in northwestern Iran on August 11, 2012. The first Mw 6.5 strike-slip earthquake, which occurred after more than 200 years of low seismicity, was followed by an Mw 6.4 oblique thrust event at an epicentral separation of about 6 km. While the first event can be associated with a distinct surface rupture, the absence of a surface fault trace and no clear aftershock signature makes it challenging to identify the fault plane of the second event. We use teleseismic body wave inversion to deduce the slip distribution in the first event. Using both P and SH waves stabilize the inversion and we further constrain the result with the surface rupture extent and the aftershock distribution. The obtained slip pattern shows two distinct slip patches with dissimilar slip directions where aftershocks avoid high-slip areas. Using the estimated slip for the first event, we calculate the induced Coulomb stress change on the nodal planes of the second event and find a preference for higher Coulomb stress on the N-S nodal plane. Assuming a simple slip model for the second event, we estimate the combined Coulomb stress changes from the two events on the focal planes of the largest aftershocks. We find that 90% of the aftershocks show increased Coulomb stress on one of their nodal planes when the N-S plane of the second event is assumed to be the correct fault plane. 相似文献
6.
《地震研究进展（英文）》2021,1(1):100007
On February 3rd, 2020, an isolated MS5.1 earthquake occurred in the northern section of the Longquanshan fault zone. This study aims at defining the geometry of seismogenic structures of this earthquake. In detail, centroid moment tensor inversion results show that the earthquake is characterized by a focal depth of 3.8 km with no corresponding surface faults. The strike/dip/rake angles for the two nodal planes are 205°/54°/96° and 15°/36°/82°, respectively. With the analyses of coseismic deformation of the surface obtained from InSAR measurements, together with the information of relocated hypocenters for a small number of aftershocks, it is concluded that a northwest-dipping nodal plane corresponds well to the source fault. The fault is suggested to have a length of about 2.8 km and a depth range of 2–5 km, and the centroid of the earthquake is located at 104.48°E and 30.71°N. Furthermore, multiple pieces of evidence indicate that this earthquake is partly driven by the overpressure effect associated with the adjacent natural gas packets, which is similar to several other moderate natural earthquakes in Sichuan Basin. 相似文献
7.
2016年11月25日新疆阿克陶地区发生的MW6.6地震,对当地人民生命造成一定的危害。基于Sentinel-1数据获取该地震的视线向同震形变场,采用贝叶斯方法反演单一断层走向为106.9°、倾角为73.8°、震源深度为17.35 km,在此断层几何模型基础上,以最速下降梯度法（Steepest Descent Method,SDM）反演滑动分布,结果表明断层面上存在两个滑动峰值,其中位于断层西侧的最大滑动量为0.66 m,深度为11.7 km,位于断层东侧的最大滑动量为0.83 m,深度为7.5 km,根据反演结果模拟LOS形变,其最大残差为~5 cm。构建倾角分别为70.79°和55.33°的双断层几何模型,并根据双断层几何模型反演了滑动分布,结果表明单一断层模型与双断层模型的滑动分布具有一致性,但是最大滑动量值有所不同,相对于单一断层模型的滑动分布而言,双断层模型的滑动量在西侧增大,其值为0.68 m;而在东侧减小,其值为0.77 m;最大残差降低了约2 cm。双断层模型库伦应力增加区域与余震的分布比较吻合。 相似文献
8.
2014年2月12日,在新疆于田县发生了里氏7.3级地震.在该地震震中附近,前人研究证明发育了大量规模不同的活动断层(如康西瓦断裂与贡嘎错断裂等).根据地震触发理论,地震发生后因地壳同震变形会导致其周边不同性质断裂破裂应力发生变化,进而影响其地震的潜在危险性.本文利用地震远场波形记录,反演了该地震滑动模型.之后,根据弹性无限半空间位错理论,计算了该地震在近场范围内活动断裂上的同震应力变化.其目的在于讨论于田地震引起的附近断裂上的库仑应力变化以及这些活动断裂可能潜在的地震危险性.在地震发生后,从国际地震学联合会(IRIS)地震数据中心,下载了震中距离介于30°~90°的地震远场波形记录,为保证台站方位角分布均匀,从中挑选了27个不同方位角的高信噪比地震记录参与理论地震图的生成和波形反演过程.我们采用广义射线理论计算生成远场理论地震波形数据.每个子断层参数的反演则利用基于全局化反演的快速模拟退火反演方法.在有限断层反演过程中,我们采用了强调波形拟合的相关误差函数作为待反演的目标函数,拟合的断层参数使目标函数为最小.之后,根据弹性无限半空间位错理论,以库仑破裂准则为基础,结合反演得到的地震震源机制解和地震位错模型,计算该地震引起的近场断层面上库仑应力的变化.由远场波形计算结果可以看到,于田地震的震源深度为10km,地震断层的倾角约71.9°,破裂面上最大的同震位移达到210cm,以左旋走滑为主并具有正倾滑分量,地震能量主要在前15s内释放.由此得到该地震的地震矩为2.91×1019 N·m,地震震级为Mw6.9.于田地震引发的余震,大致分布在三个区域内:普鲁断裂北部、康西瓦断裂东部和贡嘎错断裂中部.弹性应力计算结果表明,于田地震导致阿尔金断裂西段、普鲁断裂中段、康西瓦断裂东段和贡嘎错断裂中段的静态库仑应力明显增加,其中以康西瓦断裂东段和贡嘎错断裂中段应力增量为最大,分别达到了0.05 MPa和0.04 MPa.大量研究证明,当地震所导致的库仑应力变化大于0.01 MPa时将具有明显的地震触发作用.根据本文结果,2014年于田Mw6.9地震使普鲁断裂、贡嘎错断裂和康西瓦断裂上的库仑应力增量均超过了触发阈值,具有被触发出地震的潜在危险.因此,在以后的地震学研究中,应加强对该三条断裂地震危险性的研究和监测.此外,近6年以来,研究区域发生了3次6级以上的地震.这些地震均沿着贡嘎错断裂,由南西向北东迁移,逐步靠近阿尔金断裂,并且逐渐由正倾滑型地震转变为走滑型地震.阿尔金断裂的走滑速率达到了9mm·a-1,所以,尽管本次地震导致的阿尔金断裂库仑应力增量小于0.01 MPa,阿尔金的地震危险性也应该加强监测. 相似文献
9.
2017年8月8日四川省九寨沟县发生M_s7.0地震.本文基于Sentinel-1 SAR影像,利用InSAR技术获取了此次地震的同震形变场,反演获得同震滑动分布,计算了同震位错对余震分布和周边断层的静态库仑应力变化,并对发震构造进行了分析讨论.结果表明:①InSAR同震形变场显示,九寨沟地震造成地表形变最大量级约为20 cm(雷达视线方向),同震形变存在非对称性分布特征.②同震位错以左旋走滑为主,主要发生在4~16 km深度,最大滑动量约为77 cm,位于9 km深处.反演得到的矩震级为Mw6.46.同震错动未破裂到地表.③大部分余震发生在库仑应力增加区.此次地震增加了震中周边地区一些断裂的库仑应力,如东昆仑断裂带东段、龙日坝断裂、虎牙断裂等.④东昆仑断裂东段的未来地震危险性值得关注.⑤九寨沟地震的发震断层为树正断裂,可能是虎牙断裂的北西延伸隐伏部分,此次地震是巴颜喀拉块体南东向运动受到华南块体的强烈阻挡过程中发生的一次典型构造事件. 相似文献
10.
本文基于Sentinel-1A卫星影像数据提取了2015年皮山MW6.4地震的同震形变场, 震中北部以隆升为主, 最大抬升量为12.9 cm; 南部以沉降为主, 最大沉降量为5.5 cm。 采用基于单一断层滑动模型的多峰粒子群优化和蒙特卡罗算法, 以LOS向InSAR形变场为约束, 对发震断层的几何模型进行非线性反演。 在此基础上, 联合InSAR和GPS数据, 利用最速下降法反演断层滑动分布。 综合结果表明: 发震断层是顶部埋深约7.4 km的隐伏断裂, 断层面大小为48 km×35 km, 断层走向、 倾角、 断层滑动角分别为111°、 19°、 91°; 断层最大滑动量0.47 m, 位于深度为10.6 km的区域; 累计地震矩3.89×1018 N·m, 约合矩震级MW6.33。 最后, 依据主震断层滑移量计算了主震对周围中小断裂的库仑应力扰动变化, 结果显示距离震中最近的泽普断裂受主震影响的库仑应力明显增加; 震后3年内余震集中分布在泽普断裂库仑应力增加区域, 表明皮山地震主震对余震的发生可能具有一定的应力触发作用。 相似文献
11.
本文基于InSAR技术, 利用欧空局Sentinel-1A/ B升降轨SAR数据, 提取了2020年6月26日新疆于田MW6.3地震的同震形变场。 利用升、 降轨同震形变场约束, 分别采用MPSO算法和Bayesian方法反演此次地震发震断层均匀滑动的几何参数, 并进行对比。 然后采用SDM方法获得发震断层非均匀滑动分布, 并分析了同震库仑应力变化及其对周边断层的应力扰动。 结果表明, 同震形变场以NS向为长轴, 总体呈现西部沉降而东部隆升的特点, 而且隆升量明显小于沉降量; 滑动分布反演表明发震断层的平均滑动量为0.13 m, 平均滑动角为-104.56°, 此次地震为典型的正断破裂事件, 最大滑动量约0.55 m, 最大滑动量处滑动角为-105.2°, 位于断层倾向深度14.42 km, 释放的地震矩能量约3.65×1018 N·m, 相当于矩震级MW6.3; 同震库仑应力变化对西部琼木孜塔格断层、 硝尔库勒南缘断层等起到应力卸载作用, 对北部的木孜鲁克—鲸鱼湖断层起到应力加载作用, 结合同震库仑应力对周围断层的扰动情况, 此次地震可能对琼木孜塔格断裂带和木孜鲁克—鲸鱼湖断裂带的西端影响较大。 相似文献
12.
2010年9月4日新西兰南岛Canterbury平原发生了Mw7.1地震,震源深度约为10 km.本次地震发生在一条震前不为人所知的断层上.我们利用覆盖整个震区的合成孔径雷达(SAR)观测资料,通过干涉处理分析获得雷达视线向(LOS)同震形变场;以此资料为约束反演了断层的几何参数以及同震破裂分布.结果显示,该地震造成四条相对独立断层的破裂.大部分的地震矩释放发生在Greendale断层(编号1-4),其错动以右旋走滑为主,最大破裂约为8.5 m.其它三条断层中,经过震源的逆冲断层最大破裂为5.1 m (编号6),位于Greendale断层以西的逆冲断层最大破裂为3.5 m (编号5),位于Greendale断层北面的走滑断层最大破裂为1.9 m(编号7).反演的Greendale断层地表滑动与地质调查得到的地表破裂在形态和数值上均吻合较好.本次地震释放的地震矩为5.0×1019N·m,矩震级为7.1.板块边界带形变场分析表明,Darfield地震的发生受边界带应变分配在该地区残留构造应力场控制,其复杂性体现了区域构造应力场的特点.地震对其周围地区的应力场影响较大,库仑应力增加区与余震分布有一定对应关系,并在2011年Christchurch 6.3级地震发震断层区域造成约0.1bar的库仑应力增加,对此地震有一定的触发作用. 相似文献
13.
基于2009—2015年广东省河源市新丰江水库库区高精度定位的地震目录(ML≥1.0),划分出大坝—峡谷区的3个北西向小震密集分布带,并依据成丛小震发生在活动断裂面及其附近的原则,采用模拟退火算法和高斯-牛顿算法相结合的方法,反演了这3个小震密集带相应的断层及断层面参数,包括断层面的走向、 倾向、 倾角、 长度、 深度和地理位置,获得了大坝区北西向断裂带相关断层的成分及几何形态． 结果显示: 3条断层走向为北西—北北西,与大坝—峡谷区走向基本一致,深度为3—12 km,均为陡峭的活动断层,其长度不超过10 km, 在库区应力场作用下均以走滑为主兼少许垂直错动; 大坝附近为几条断层端点与断层相切点的汇集区,区域应力易集中于此而成为库区地震最活跃的部位． 此外,根据断层反演结果及前人资料,论证了白田—双塘断层为新丰江1962年MS6.1地震的发震构造,并首次发现河源断裂在白田至双塘之间中断了约5 km,中断的断裂构造为白田—双塘断层的一部分． 相似文献
14.
南汀河断裂带是滇西南块体内部的一条左旋走滑断裂带,几乎横切整个块体,总长度达380km,是块体内NE向断裂中最长的一条,也是次级块体的边界断裂.南汀河断裂带晚第四纪活动性非常强烈,但仅南段在1941年记录到一次约7级的地震,其余段落还没有5级以上地震的记录,目前可能正处于应力积累和孕震阶段.2014年10月7日发生的景谷MS6.6地震位于断裂带南东约94km,其地震烈度等震线长轴与余震皆呈北西展布,指向南汀河断裂带.为了解景谷地震对周边构造特别是南汀河断裂带的影响,本文通过数值模拟方法计算了地震触发的同震静态库仑应力变化.利用两种同震滑动分布模型计算获得的结果显示,景谷地震对震中附近的断裂,如澜沧江断裂和景谷断裂影响较大,局部应力增加可达90kPa;对较远的断裂,如南汀河断裂带、龙陵—澜沧断裂带和无量山断裂带的影响较小,应力变化值均小于10kPa.通过设置不同断层参数进一步计算,南汀河断裂带北段两支断裂断层面上的静态库仑应力扰动呈半圆形分布,应力增加的最大值位于24.15°N附近的地表,沿断层的走向和深度都逐渐减小.其中西支断裂上应力变化最大值为0.89kPa,东支断裂上为1.18kPa.此外,在南汀河断裂带北段的古地震研究结果显示,该断裂段全新世以来发生过产生地表破裂的大地震,震级应当不低于7级.放射性碳测年将该次古地震事件的发震时间限定在900—1480AD,离逝时间为535—1115年.结合古地震事件的离逝时间和断裂带的滑动速率,本文计算得到南汀河断裂带北段已经积累的水平滑动量为2.8+1.5/-1.0m,进一步利用滑动量与震级的经验公式可估算出该断裂段目前积累的滑动量如果完全释放将会产生一个7.5+0.1/-0.2级的地震.虽然景谷地震在南汀河断裂带上触发的静态库仑应力变化值表明,该地震可能不会引起南汀河断裂带地震危险性的突变,但仍起到一定的加速作用.再考虑到断裂带北段目前已经积累了约7.5级地震所需的能量,该断裂段在未来具有较高的地震危险性. 相似文献
15.
2013年7月22日,在甘肃岷县漳县交界处发生MS6.6地震,地震震中位置靠近临潭—宕昌断裂.本文通过构建有限断层模型,利用国家强震动台网中心提供的12条强地面运动三分量资料,通过波形反演方法来研究这次地震的震源破裂过程.结果显示这次地震是发生在甘东南地区岷县—宕昌断裂带东段附近的一次MW6.1级逆冲兼具左旋走滑破裂事件,最大滑动量约为80cm.发震断层走向及滑动性质与岷县—宕昌断裂吻合,推断本次地震与东昆仑断裂向北的扩展和推挤密切相关,是岷县—宕昌断裂进一步活动的结果. 相似文献
16.
本文利用GPS观测对丽江—小金河断裂带的现今断层运动和变形状态进行了分析和探讨.丽江—小金河断裂带两侧地块地壳变形差异显著,GPS速度剖面结果显示断裂带两侧存在地壳变形不连续现象;进一步以GPS速度场为约束,基于负位错模型反演的丽江—小金河断裂带的断层闭锁空间分布结果显示,以木里为界,北东段断层强闭锁从地表向深部延伸至15km左右,西南段断层闭锁程度较高的区域位于5～15km范围内,浅层表现为弱闭锁的状态;滑动亏损速率结果显示,两闭锁段的滑动亏损速率相差近4mm·a~(-1),说明丽江—小金河断裂带西南段的背景滑动速率明显高于北东段.基于数值模拟分析了西南段浅层蠕滑运动对周边断层的影响,结果表明西南段的浅层左旋滑动对北东段闭锁区和西南段深部强闭锁区均为正影响. 相似文献
17.
《Earth and Planetary Science Letters》2006,241(1-2):336-350
We investigated the fault geometry effects and the corresponding coseismic slip distribution using various proposed earthquake fault models for the Chi-Chi earthquake of 21 September 1999. The types of fault geometries are threefold: a simple planar fault plane, a two segmented planar fault plane and a three dimensional (3D) curved fault surface rupture propagation model. We derived the estimated spatial slip distribution from an inversion analysis of GPS coseismic displacement data and show that the 3D fault model is the preferred solution. The simple and segmented fault models lead to significant artificial slip distributions associated with the pre-defined fault geometry and the spatial distribution of GPS stations. The spatial distribution of coseismic slip deduced from the 3D fault model has three observable features: (1) the overall slip is concentrated at depth of less than 12 km, which may well correspond to a shallow-dipping detachment; (2) the maximum slip of about 10 m is located 45 km to the north of the epicenter; and (3) the slip vector is dominated by the dip-slip component. In addition, the results from the inversion of GPS data are consistent with those from the inversion analysis of teleseismic broadband data. A resolution analysis, further, demonstrates that the results are highly correlated with field GPS data studies when we used synthetic test data. The inversion of spatially distributed GPS data is highly sensitive to fault geometry. We conclude that the use of the 3D fault model is not only necessary but also certainly competent enough to well explain the inferred slip style and the observed static coseismic displacements. 相似文献
18.
Athanassios Ganas Zafeiria Roumelioti Vassilios Karastathis Konstantinos Chousianitis Alexandra Moshou Evangelos Mouzakiotis 《Journal of Seismology》2014,18(3):433-455
We investigate mainshock slip distribution and aftershock activity of the 8 January 2013 M w?=?5.7 Lemnos earthquake, north Aegean Sea. We analyse the seismic waveforms to better understand the spatio-temporal characteristics of earthquake rupture within the seismogenic layer of the crust. Peak slip values range from 50 to 64 cm and mean slip values range from 10 to 12 cm. The slip patches of the event extend over an area of dimensions 16?×?16 km2. We also relocate aftershock catalog locations to image seismic fault dimensions and test earthquake transfer models. The relocated events allowed us to identify the active faults in this area of the north Aegean Sea by locating two, NE–SW linear patterns of aftershocks. The aftershock distribution of the mainshock event clearly reveals a NE–SW striking fault about 40 km offshore Lemnos Island that extends from 2 km up to a depth of 14 km. After the mainshock most of the seismic activity migrated to the east and to the north of the hypocenter due to (a) rupture directivity towards the NE and (b) Coulomb stress transfer. A stress inversion analysis based on 14 focal mechanisms of aftershocks showed that the maximum horizontal stress is compressional at N84°E. The static stress transfer analysis for all post-1943 major events in the North Aegean shows no evidence for triggering of the 2013 event. We suggest that the 2013 event occurred due to tectonic loading of the North Aegean crust. 相似文献
19.
利用1999—2015年GPS水平速度场, 基于块体-位错模型, 反演了青藏高原东北缘4条主要断裂(海原断裂, 六盘山断裂, 陇县—宝鸡断裂, 西秦岭北缘断裂)的闭锁程度和滑动亏损速率的空间分布, 并分析了各断裂的地震危险性。 结果显示, 六盘山断裂南段、 陇县-宝鸡断裂北段、 西秦岭北缘断裂东段闭锁程度最强, 闭锁深度达到24 km左右; 西秦岭北缘断裂东段滑动亏损速率最大, 平均值达到3 mm/a; 六盘山断裂南段、 陇县—宝鸡断裂北段滑动亏损速率平均值达到1.9 mm/a, 稍弱于西秦岭北缘断裂东段; 海原断裂闭锁程度和滑动亏损速率相对较小, 闭锁程度和滑动亏损都仅分布在浅部。 我们认为现阶段海原断裂的地震危险性相对较小, 六盘山断裂南段、 陇县—宝鸡北段、 西秦岭北缘断裂东段地震危险性高于这些断裂的其他段落。 这些结果对于青藏高原东北缘地震危险性判定和地震灾害评估具有参考意义。 相似文献
20.
2017年8月8日的九寨沟MS7.0地震发生在岷江断裂、塔藏断裂及虎牙断裂交汇地区,地处青藏高原东北部的川甘交界地区,位于巴颜喀拉地块的东缘,地质构造复杂,对于九寨沟地震震中位置和发震断层的确定,存在不同意见.本文利用GNSS及升降轨InSAR观测,在获取九寨沟地震同震形变场的基础上,基于均匀弹性半无限位错模型,联合反演了发震断层的滑动分布模型,并计算了同震库仑应力变化.InSAR同震形变场显示,视线向最大沉降量和抬升量分别为0.21 m和0.16 m,形变场长轴为NW向,形变主要集中在断层西侧.距震中40 km和65 km的九寨和松潘两县,水平向的GNSS同震位移分别达14.31 mm和8.22 mm.联合GNSS和InSAR同震形变场反演得到的滑动分布主要集中在沿走向5~33 km,倾向2~20 km的范围内,平均滑动量为0.18 m,最大滑动量为0.91 m.发震断层长40 km,宽30 km,走向155°,倾角81°,滑动角-9.56°.同震位移场及滑移分布模型表明此次地震为一次左旋走滑为主的地震事件,地震破裂并未完全到达地表,与虎牙断裂北段的几何产状和运动学性质更为接近,结合精定位余震的分布,我们确定虎牙断裂北段为此次地震的发震断层,震中位于北纬33.25°,东经103.82°,震源深度10.86 km,矩震量为7.754×1018 Nm,相应的矩震级为MW6.5,与美国地调局和哈佛大学给出的震源机制解基本一致.同震库仑应力导致了虎牙断裂北段延长线的东北和西南两端应力增强,其中塔藏断裂的罗叉段和马磨段未来强震的危险性值得关注. 相似文献