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1.
The new inversion algorithm developed based on the recent progress in the nonlinear programming study by us is used to invert the earthquake source process of Chi Chi earthquake Mw7.6, 20 Semptember,1999, Taiwan. A curve fault model is constructed in our inversion to make the fault model close to the real rupturing fault to reduce the influence from the discrepancy between the constructed fault model and the real rupturing fault. The results show that (1) the rupture process of the Chi Chi earthquake source lasted about 32 seconds and the main faulting occurred between 6th to 21st second after the start of the ruptures and the high slip area were mainly located at the northern segment of the fault. (2) The slip was dominated by thrust faulting. The average rake angle was 64.5°, which was very consistent with those inverted by USGS, Harvard and CWB (Central Weather Bureau of Taiwan). The amount of the moment inverted in this paper was 7.76×1020 NM, which was a slightly bigger than those inverted by USGS and Harvard. (3) A clear nucleation step existed in the source faulting process and it lasted about 6 seconds. The moment release rate accelerated obviously at the end of the nucleation step. The faulting started from the southern segment and mainly occurred at the northern segment after 10 seconds. At the end of this paper, we analyzed the reliability of the inversion result via comparing with the GPS observations and discussed its scientific signification. 相似文献
2.
《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
3.
We propose an inversion scheme for retrieval of characteristics of seismic point sources, which in contrast to common practice,
takes into account anisotropy. If anisotropy is neglected during inversion, the moment tensors retrieved from seismic waves
generated by sources situated in anisotropic media may be biased. Instead of the moment tensor, the geometry of the source
is retrieved directly in our inversion; if necessary, the moment tensor can be then determined from the source geometry aposteriori.
The source geometry is defined by the orientation of the slip vector and the fault normal as well as the strength of the event
given by the size of the slip and the area of the fault. This approach allows direct interpretation of the source geometry
in terms of shear and tensile faulting. It also makes possible to identify volumetric source changes that occur during rupturing.
We apply the described algorithm to one event of the 2000 West Bohemia earthquake swarm episode. For inversion we use information
of the direct P waves. The structure is approximated by three different models determined from travel-time observations. The
models are inhomogeneous isotropic, inhomogeneous anisotropic, and homogeneous anisotropic. For these models we obtain seismic
moments MT = 3.2 − 3.8 × 1014 Nm and left-lateral near-vertical oblique normal faulting on a N-S trending rupture surface. The orientation of the rupture
surface is consistent with fault-plane solutions of earlier studies and with the spatial distribution of other events during
this swarm. The studied event seems to be accompanied by a small amount of crack opening. The amount of crack opening is slightly
reduced when the inhomogeneous anisotropic model is assumed, but it persists. These results and additional independent observations
seem to indicate that tensile faulting occurs as a result of high fluid pressure. 相似文献
4.
Introduction An earthquake of MS=7.8 occurred near the Gujarat of India on January 26, 2001, which was one of the most deadly earthquakes since there was the record in the Indian history (Bendick, et al, 2001; Gupta, et al, 2001). The USGS of USA determined the origin time of the earthquake to be 3h16min41s (UTC), and the epicenter location to be 70.32篍, 23.40篘. Shortly after the earthquake, the moment tensor solutions or focal mechanisms and other related parameters were offered by s… 相似文献
5.
The Chi‐Chi earthquake (MW = 7.6) took place in central western Taiwan in 1999. The earthquake caused reactivation of the Chelungpu Fault and resulted in 100‐km‐long surface ruptures. The fault strikes mostly north–south to NNE–SSW; however, the northern tip of the southern segment of the surface ruptures rotates clockwise to define an east–west trend, then jumps to a shorter NNW‐trending rupture. The largest vertical displacement is recorded in the Shihkang area of the Shihkang–Shangchi Fault Zone, where vertical slips are up to 8–10 m. The Shihkang–Shangchi Fault Zone displays a complex fault pattern as a linkage damage zone between two fault segments with the greatest concentration of faults and fractures. Our new interpretation, based on recent published geometric, kinematic, and geophysical studies on the Chi‐Chi earthquake fault, suggests that the Shihkang–Shangchi Fault Zone is not a simple termination zone, but may be an ‘overstep zone’ or a ‘transfer zone’. Slip analysis along the surface ruptures indicates that they are composed of three fault segments and the amount of slip partly depends on the intersection angle between slip direction and fault strike. Our numerical modeling for the area indicates that Coulomb stress changes are mainly concentrated on tips and bends of the surface ruptures. Slip patterns indicate that the fault propagates toward the northeast. Therefore, this study suggests high potential for future earthquake activity along the unruptured Shangchi segment. Hence, future geohazard studies should focus on the Shangchi segment to evaluate potential earthquakes, determine recurrence intervals, and reduce future earthquake hazards. 相似文献
6.
The source parameters, such as moment tensor, focal mechanism, source time function (STF) and temporal-spatial rupture process,
were obtained for the January 26, 2001, India, M
S=7.8 earthquake by inverting waveform data of 27 GDSN stations with epicentral distances less than 90°. Firstly, combining
the moment tensor inversion, the spatial distribution of intensity, disaster and aftershocks and the orientation of the fault
where the earthquake lies, the strike, dip and rake of the seismogenic fault were determined to be 92°, 58° and 62°, respectively.
That is, this earthquake was a mainly thrust faulting with the strike of near west-east and the dipping direction to south.
The seismic moment released was 3.5×1020 Nm, accordingly, the moment magnitude M
W was calculated to be 7.6. And then, 27 P-STFs, 22 S-STFs and the averaged STFs of them were determined respectively using
the technique of spectra division in frequency domain and the synthetic seismogram as Green’s functions. The analysis of the
STFs suggested that the earthquake was a continuous event with the duration time of 19 s, starting rapidly and ending slowly.
Finally, the temporal-spatial distribution of the slip on the fault plane was imaged from the obtained P-STFs and S-STFs using
an time domain inversion technique. The maximum slip amplitude on the fault plane was about 7 m. The maximum stress drop was
30 MPa, and the average one over the whole rupture area was 7 MPa. The rupture area was about 85 km long in the strike direction
and about 60 km wide in the down-dip direction, which, equally, was 51 km deep in the depth direction. The rupture propagated
50 km eastwards and 35 km westwards. The main portion of the rupture area, which has the slip amplitude greater than 0.5 m,
was of the shape of an ellipse, its major axis oriented in the slip direction of the fault, which indicated that the rupture
propagation direction was in accordance with the fault slip direction. This phenomenon is popular for strike-slip faulting,
but rather rare for thrust faulting. The eastern portion of the rupture area above the initiation point was larger than the
western portion below the initiation point, which was indicative of the asymmetrical rupture. In other words, the rupturing
was kind of unilateral from west to east and from down to up. From the snapshots of the slip-rate variation with time and
space, the slip rate reached the largest at the 4th second, that was 0.2 m/s, and the rupture in this period occurred only
around the initiation point. At the 6th second, the rupture around the initiation point nearly stopped, and started moving
outwards. The velocity of the westward rupture was smaller than that of the eastward rupture. Such rupture behavior like a
circle mostly stopped near the 15th second. After the 16th second, only some patches of rupture distributed in the outer region.
From the snapshots of the slip variation with time and space, the rupture started at the initiation point and propagated outwards.
The main rupture on the area with the slip amplitude greater than 5 m extended unilaterally from west to east and from down
to up between the 6th and the 10th seconds, and the western segment extended a bit westwards and downwards between the 11th
and the 13th seconds. The whole process lasted about 19 s. The rupture velocity over the whole rupture process was estimated
to be 3.3 km/s.
Foundation item: 973 Project (G1998040705) from Ministry of Science and Technology, P. R. China, and the National Science Foundation of China
under grant No.49904004.
Contribution No. 02FE2026, Institute of Geophysics, China Seismological Bureau. 相似文献
7.
联合近场GPS测站1-Hz运动学位移、 强震仪加速度波形和全球台站P震相波形作为约束, 以时空滑动分布约束条件和ABIC模型参数选择方法, 结合先验的滑动方向变化范围, 反演2008年汶川MS8.0地震的震源时空破裂过程, 给出了能够综合反映震源破裂过程的统一模型。 结果表明, 汶川地震总体上存在4个主要的破裂区, 最主要的一个破裂区位于震源东北40~120 km, 断层面上的最大位错量约为10 m, 主体滑动分布在2~20 km深度范围, 破裂达到地表; 第二个主体破裂区位于断层破裂带南段, 最大滑动量达到6 m; 另外2个主体滑动区位于断层破裂带北段, 但滑动破裂量小于断层南段破裂区的滑动量, 滑动破裂值最大值为4 m, 超过1 m的区域在走向上超过70 km。 反演得到的断层滑动模型的地震矩为9.5×1021 Nm, 相应的矩震级为MW7.95。 汶川地震破裂表现为单侧破裂, 起始破裂在汶川下方16 km深度, 向东北方向一致性地传播, 过程持续~120 s。 在地震发生后0~10 s内, 破裂集中在震源起始破裂区, 滑动破裂值为~1.0 m, 之后破裂向东北方向扩展, 震后20~40 s是主要的破裂时段。 在40~60 s, 破裂跨越断层南段和北段。 在80~90 s破裂最大值开始下降, 在100~110 s时, 下降为~0.5 m, 在110~120 s时, 下降为~0.1 m。 加入近场GPS测站1-Hz 波形数据与近场强震仪波形和远场长周期体波联合反演, 提高了震源破裂模型的空间分辨率, 特别是浅部滑动破裂区的分辨率, 反演的最大滑动破裂值比不用1-Hz 波形数据反演的结果增大, 表明近场1-Hz GPS波形数据对于揭示汶川地震的时空破裂过程具有重要的作用。 相似文献
8.
Long period body waves data recorded by the China Digital Seismograph Network (CDSN) are inverted for the seismic moment tensors
of the April 26, 1990, Gonghe, QinghaiM
S=6.9 earthquake and itsM
S=5.0 after-shock occurred on May 7, 1990. In the inversion, the generalized reflection-transmission coefficient matrix method
is used to generate Green’s function. From the inversion it is obtained that the rupture process of theM
S=5.0 aftershock is relatively simple, and that of the main shock is rather complex. There are at least two events during main
shock rupture process with an interval about 35 seconds. The focal mechanisms of two events are roughly the same as that of
the aftershock, all of them were mainly reverse dip-slipping faulting with minor left-lateral strike-slip motion. These results
indicate that the Gonghe earthquake was the result of the farther extension of one NWW-SEE striking buried fault on the southern
margin of Gonghe basin from shallower depth to deeper depth and from NW to SE under the action of a nearly horizontal NE direction
compressive stress.
Contribution No. 95A0111, Institute of Geophysics, SSB, China. 相似文献
9.
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
10.
2008年5月12日,青藏高原东缘龙门山断裂带发生汶川MW7.9地震,该地震使得北川—映秀断裂、灌县—江油断裂发生了同震破裂。本文主要利用震后通过复测获得的GPS同震形变场,采用Yabuki&Matsu’ura反演计算方法和分段平面断层模型,反演了地震同震滑动分布。结果表明:映秀—北川主破裂带的断层错动,在映秀附近以逆冲滑动为主,而在北川以北,其走滑运动明显大于逆冲,这一结果与震后地质调查结果与通过地震波研究获得的断层破裂特征相一致;反演得到的最大滑动量达到9.3m和9.6m,分别对应于这次地震中地表破坏最为严重的北川和映秀地区;由所获得的滑动分布计算的地震矩为8.07×1020 N.m,对应的震级为MW7.9。研究结果初步显示,Yabuki&Matsu’ura反演方法可适用在内陆地震断层反演计算中。 相似文献
11.
用近震源波形资料拟合反演地震的震源破裂过程,所包含的一些不确定因素将对反演结果的精度及可靠性产生影响,文中的数值实验分析了所假定的反演断层模型参数的某些不确定性对反演结果的影响程度,并对观测波形的截取长度对反演精度的影响进行了讨论．结果表明：(1)近震源地震波形资料能较好地分辨断层浅部的破裂过程.然而对断层深部的位错分布的约束和反演能力较差．联合使用近、远场地震波资料进行反演,能反演出一个更为完全的整个断层破裂过程的图像.(2)用近震源地震波资料反演时,反演结果对所假定的反演断层的走向和倾角非常敏感.断层走向偏离真实值2°或倾角偏离真实值5°都会导致一个虚假的反演结果.(3)反演中所使用的介质速度结构模型的不确定性,也会对反演结果产生影响. 相似文献
12.
Introduction On November 14, 2001, a great earthquake occurred in the western Kunlun Mountain area(Figure 1). The original time is 09h26min10.0s (UTC); the hypocentral location is 35.95°N,90.54°E; focal depth is 10 km from USGS National Earthquake Information Center (NEIC);MS=8.1 from China Seismic Network and Mw=7.8 from Harvard and Earthquake Research Insti-tute (ERI), University of Tokyo. This earthquake, known as the western Kunlun Mountain earth-quake, is an extraord… 相似文献
13.
1997年11月8日西藏玛尼Mw75级地震是干涉雷达技术应用于地震观测以来的一次重要事件.Peltzer等认为该形变场体现了地壳的非线性弹性形变响应，挤压象限和拉张象限的杨氏模量比值为2.相同的情形并没有在其他地震同震形变场中发现，通常用线弹性理论就能够很好地解释观测数据.考虑到他们所用断层模型的简化程度和纯走滑约束等，本研究认为非线性弹性解释是牵强的.应用广泛使用的Okada线弹性位错模型，采用卫星观测得到的地表断层位置，去除倾滑为零的约束，基于非线性优化反演方法寻求拟合雷达观测的最佳断层几何参数和均匀滑动参数.结果表明，线弹性模型能够满意解释观测数据.断层在朝阳湖以东的段落最深达到165 km，随着断层向两侧延伸，深度逐渐减小；反演得到的断层倾 相似文献
14.
Based on digital teleseismic P-wave seismograms recorded by 28 long-period seismograph stations of the global seismic network,
source process of the November 14, 2001 western Kunlun Mountain M
S=8.1 (M
W=7.8) earthquake is estimated by a new inversion method. The result shows that the earthquake is a very complex rupture event.
The source rupture initiated at the hypocenter (35.95°N, 90.54°E, focal depth 10 km, by USGS NEIC), and propagated to the
west at first. Then, in several minutes to a hundred minutes and over a large spatial range, several rupture growth points
emerged in succession at the eastern end and in the central part of the finite fault. And then the source rupture propagated
from these rupture growth points successively and, finally, stopped in the area within 50 km to the east of the centroid position
(35.80°N, 92.91°E, focal depth 15 km, by Harvard CMT). The entire rupture lasted for 142 s, and the source process could be
roughly separated into three stages: The first stage started at the 0 s and ended at the 52 s, lasting for 52 s and releasing
approximately 24.4% of the total moment; The second stage started at the 55 s and ended at the 113 s, lasting for 58 s and
releasing approximately 56.5% of the total moment; The third stage started at the 122 s and ended at the 142 s, lasting for
20 s and releasing approximately 19.1% of the total moment. The length of the ruptured fault plane is about 490 km. The maximum
width of the ruptured fault plane is about 45 km. The rupture mainly occurred within 30 km in depth under the surface of the
Earth. The average static slip in the underground rocky crust is about 1.2 m with the maximum static slip 3.6 m. The average
static stress drop is about 5 MPa with the maximum static stress drop 18 MPa. The maximum static slip and the maximum stress
drop occurred in an area within 50 km to the east of the centroid position.
Foundation item: Joint Seismological Science Foundation of China (103066) and Foundation of the Seismic Pattern and Digital Seismic Data
Application Research Office of Institute of Earthquake Science of the China Earthquake Administration. 相似文献
15.
2016年4月15日16时25分（UTC）,日本熊本县发生MW7.1强烈地震,给当地人员、建筑及经济造成严重灾难和巨大损失.日本地震观测网F-net给出的震源机制解显示此次地震的震源位置为130.7630°E,32.7545°N,深度12.45 km,节面Ⅰ：走向N131°E、倾角53°、滑动角-7°;节面Ⅱ：走向N226°E、倾角84°、滑动角-142°.与此同时,余震的震中分布及其震源机制结果显示主震的震源机制在破裂过程中有可能发生了变化,单一的震源机制不足以充分解释观测数据.本文依据GNSS和InSAR地表形变反演结果为约束,并结合活动构造资料为参考,构建了震源机制变化的有限断层模型,采用水平层状介质模型,利用日本强震观测台网K-NET和KiK-net的近场加速度观测记录,通过多时间窗线性波形反演方法反演了此次地震的震源破裂过程.研究结果显示,这是一次沿Futagawa-Hinagu断层带发生的右旋走滑破裂事件,发震断层分为南北两段,其中北段走向N235°E、倾角60°,南段走向N205°E、倾角72°,断层深度范围和余震深度分布基本一致,断层面上滑动主要集中于断层北段,最大滑动量约7.9 m,整个断层的破裂过程持续约18 s,释放地震矩5.47×1019 N·m（MW7.1）. 相似文献
16.
本文提出了一种基于恒定破裂速度和固定子事件震源时间函数的假定、利用远场地震波形资料获取大地震震源机制的时空变化图像的线性反演方法,并利用这种方法及全球范围内48个台站的长周期波形资料反演建立了2008年汶川MS8.0地震的震源机制随时间和空间变化的图像.根据这个图像可知,汶川大地震断层的西南端震源机制接近于逆冲,随着破裂向东北方向延伸,震源机制的走滑分量逐渐增大,走滑分量超过逆冲分量的转折点在震中东北大约190 km的位置.为了检验反演方法的有效性和反演结果的可靠性,我们特别设计了一个数值试验对反演结果进行了检验.检验结果表明,我们在本文中提出的反演方法是有效的,关于汶川大地震的反演结果也是可靠的（除长周期信号较弱的一段外).通过比较发现,反演结果与震后野外考察的结果也相当吻合. 相似文献
17.
1999年9月21日（当地时间）台湾集集7.6级地震是一个逆断层型地震．用回归分析法对台湾集集地震的加速度峰值数据进行分析，得出了这次地震的水平与垂直向的加速度峰值衰减关系．从残差分布上看，位于断层上盘和下盘上的加速度峰值与从衰减关系所得到的结果相比存在不同的系统偏差，断层上盘地表的加速度峰值较高，而下盘地表的加速度峰值较低．从这次地震的加速度峰值分布等值线图上也可以看出，加速度峰值的分布相对于断层呈现明显的不对称性，上盘衰减较慢而下盘衰减较快．在近断层强地面运动研究、地震危险性分析、设定地震研究与震害预测等工作中，应考虑可能地震的震源机制特点，以便使所用的衰减模型更能反映不同地震环境地区的地震动分布特征． 相似文献
18.
利用1999—2007期GPS水平速度场数据,采用Defnode负位错反演程序估算了龙门山断裂在汶川地震前的闭锁程度和滑动亏损分布,结合龙门山断裂带附近地表水平应变率场结果,综合分析了震前地壳变形特征.反演结果表明,震前龙门山断裂中北段处于完全闭锁状态,闭锁深度达到21 km(闭锁比例0.99)左右,垂直断层方向的挤压滑动亏损速率约为2.2 mm/a,平行断层方向的右旋滑动亏损速率约为4.6 mm/a.龙门山断裂南段只有地表以下12 km闭锁程度较高(闭锁比例0.99),垂直断层方向滑动亏损速率约为1.4 mm/a,平行断层方向滑动亏损速率约为4.6 mm/a;在12~16 km处闭锁比例约为0.83,垂直断层方向滑动亏损速率约为1.2 mm/a,平行断层方向滑动亏损速率约为3.8 mm/a;在16~21 km处闭锁比例约为0.75,垂直断层方向滑动亏损速率约为1.1 mm/a,平行断层方向滑动亏损速率约为3.5 mm/a.在21~24 km处整条断裂均逐步转变为蠕滑.上述反演结果与区域应变计算获得的龙门山断裂带中北段整体应变积累速率较低、南段应变积累速率较高相一致,均表明中北段闭锁程度高、南段闭锁程度稍低,该特征可以较好地解释汶川地震时从震中向北东向单向破裂现象. 相似文献
19.
Source process of the 1990 Gonghe,China, earthquake and tectonic stress field in the northeastern Qinghai-Xizang (Tibetan) plateau 总被引：13，自引：0，他引：13
TheM
s
=6.9 Gonghe, China, earthquake of April 26, 1990 is the largest earthquake to have been documented historically as well as recorded instrumentally in the northeastern Qinghai-Xizang (Tibetan) plateau. The source process of this earthquake and the tectonic stress field in the northeastern Qinghai-Xizang plateau are investigated using geodetic and seismic data. The leveling data are used to invert the focal mechanism, the shape of the slipped region and the slip distribution on the fault plane. It is obtained through inversion of the leveling data that this earthquake was caused by a mainly reverse dip-slipping buried fault with strike 102°, dip 46° to SSW, rake 86° and a seismic moment of 9,4×1018 Nm. The stress drop, strain and energy released for this earthquake are estimated to be 4.9 MPa, 7.4×10–5 and 7.0×1014 J, respectively. The slip distributes in a region slightly deep from NWW to SEE, with two nuclei, i.e., knots with highly concentrated slip, located in a shallower depth in the NWW and a deeper depth in the SEE, respectively.Broadband body waves data recorded by the China Digital Seismograph Network (CDSN) for the Gonghe earthquake are used to retrieve the source process of the earthquakes. It is found through moment-tensor inversion that theM
s
=6.9 main shock is a complex rupture process dominated by shear faulting with scalar seismic moment of the best double-couple of 9.4×1018 Nm, which is identical to the seismic moment determined from leveling data. The moment rate tensor functions reveal that this earthquake consists of three consecutive events. The first event, with a scalar seismic moment of 4.7×1018 Nm, occurred between 0–12 s, and has a focal mechanism similar to that inverted from leveling data. The second event, with a smaller seismic moment of 2.1×1018 Nm, occurred between 12–31 s, and has a variable focal mechanism. The third event, with a sealar seismic moment of 2.5×1018 Nm, occurred between 31–41 s, and has a focal mechanism similar to that inverted from leveling data. The strike of the 1990 Gonghe earthquake, and the significantly reverse dip-slip with minor left-lateral strike-slip motion suggest that the pressure axis of the tectonic stress field in the northeastern Qinghai-Xizang plateau is close to horizontal and oriented NNE to SSW, consistent with the relative collision motion between the Indian and Eurasian plates. The predominant thrust mechanism and the complexity in the tempo-spatial rupture process of the Gonghe earthquake, as revealed by the geodetic and seismic data, is generally consistent with the overall distribution of isoseismals, aftershock seismicity and the geometry of intersecting faults structure in the Gonghe basin of the northeastern Qinghai-Xizang plateau.Contribution No. 96 B0006 Institute of Geophysics, State Seismological Bureau, Beijing, China. 相似文献
20.
2008年10月6日16时30分(北京时间),西藏自治区拉萨市当雄县发生Ms6.6级地震.震中位于亚东-谷露近南北向裂谷带北段,是该活动构造带近年来发生的一次较大地震.我们利用中国地震台网中心(CENC)和美国地震学联合研究所(IRIS)提供的宽频带地震记录资料,基于点源和有限断层模型,通过波形拟合反演了该地震的震源过程.结果表明,本次地震的发震断层面走向为183.3°,倾角为49.5°,滑动角约为－115°,最大滑动量达130 cm,地震震源的深度为9.6 km,地震的标量地震矩为2.85×1018 N·m,破裂持续时间约10 s.根据地震破裂的几何学和运动学特征,推测该地震主要发生在亚东-谷露南北向裂谷活动构造带内的一个高角度西倾断层上,是一个以拉张为主且有一定的右旋分量的破裂事件,这与青藏高原现今GPS测量所揭示的该地区地壳运动特征基本一致,暗示了青藏高原南部从西向东地表运动从北北东向到南东东向的运动学转变所导致的地壳在近东西方向上的拉张变形特征. 相似文献