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1.
四川汶川MS 8.0大地震地表破裂带的遥感影像解析 总被引：21，自引：1，他引：20
2008年5月12日发生于四川盆地西部龙门山断裂带的汶川MS 8.0级大地震造成巨大的人员伤亡和财产损失,并形成了空间上基本连续分布的地表破裂带（地震断层）。根据地表破裂带的解译标志及影像特征,我们充分利用震后中国科学院航空遥感飞机所获取的高分辨率航空遥感图像以及我国台湾福卫-2卫星遥感图像进行详细解译分析,并结合震后的多次野外科学考察与验证,初步查明了四川汶川MS 8.0级大地震所产生地表破裂带的空间分布特征。遥感解译分析表明汶川大地震产生的地表破裂带总计长约300 km,其几何学特征十分复杂,主要沿先存的NE走向活动断裂带呈不连续展布;变形特征以逆冲挤压为主兼具右旋走滑分量。按同震地表破裂带所在断裂带位置,可将其分为两条： 中央地表破裂带：沿映秀-北川断裂带分布,从西南开始呈北东向延伸至平武县水观乡石坎子北东一带,长约230 km,最大垂直位移量达6.0 m左右,最大右旋水平位移达5.8 m;山前地表破裂带：沿灌县-安县断裂带分布,由都江堰市向峨乡一带开始呈北东向延伸至安县雎水镇一带,长约70 km,以逆冲挤压为主,最大垂直位移量可达2.5 m。此外,遥感图像分析还表明上述地表破裂带与地质灾害分布在空间上具有十分密切的相关性,因此,挤压逆冲-走滑型地震断层的致灾效应研究是未来应该加以重视的研究课题。 相似文献
2.
东亚陆缘带构造扩张的深部热力学机制 总被引：6，自引：2，他引：6
近年来,我国地球科学家提出“陆缘构造扩张”观点,较好的解释了亚洲东部大陆边缘于新生代发生扩张离散运动的原因。本文基于“陆缘构造扩张”观点,探讨东亚陆缘带构造扩张的深部热力学机制。东亚陆缘带是具有强烈岩浆活动和构造变形的扩张带,此构造带的主要地球物理特征是频繁的地震活动和明显的地热异常。东亚陆缘扩张带地震层析成像显示,太平洋板块低角度俯冲到欧亚板块之下并平卧于670km相变界面之上。这种图像可能是俯冲后撤导致陆缘扩张的结果。热模拟及地球动力学计算表明:俯冲后撤时间距今约76Ma,海沟带后撤为陆缘壳体的生长留下空间,并形成东亚陆缘壳体增生扩展的前沿带,陆缘扩张量约700km。 相似文献
3.
阿留申俯冲带位于环太平洋俯冲带最北端,是东太平洋型俯冲和西太平洋俯冲的过渡区域。该俯冲带火山岛弧距离海沟的距离从东向西逐渐增大,而形成地球上独特的岛弧火山链与海沟V字型斜交的现象。这一现象的运动学成因目前并没有统一的认识。本文通过对阿留申俯冲带几何形态数据、运动学数据进行整理分析,尝试运用构造赤道理论探讨该现象形成的运动学背景。阿留申俯冲带的几何学数据表明:从俯冲带东段(175°E)至俯冲带西段(155°W),火山岛弧距俯冲海沟的距离从80 km增加至250 km。与此同时,俯冲板片的倾角由60°减小至30°。板块的运动学分析表明:相对北美板块,太平洋板块的东段的运动矢量为48 mm/a,向北运动;逐渐转变为西段的78mm/a,向西北方向运动。相对于软流圈,太平洋板块的运动方向没有改变,始终向西北方向运动,速率向西逐渐增加。因此,在俯冲带的东段太平洋板块的绝对运动方向和相对运动方向存在30°左右的夹角,而这个夹角在西段几乎不存在。太平洋板块的绝对运动方向和相对运动方向之间的夹角不同,会导致软流圈对俯冲板片的反作用力差异,从而形成不同的俯冲角度和俯冲带宽度。太平洋板块相对北美板块和相对地幔的速度方向夹角的变化被认为是引起阿留申火山弧与海沟"V"字型斜交的运动学成因。 相似文献
4.
缅甸Sagaing走滑断裂及对睡宝盆地构造演化的控制和影响 总被引：5，自引：0，他引：5
在研究Sagaing走滑断裂的形成和发展的基础上将其分为2个阶段:第一阶段古新世—早始新世洋陆俯冲造成了缅甸板块与欧亚板块的分离,使缅甸板块加速向北漂移,Sagaing断裂开始形成;第二阶段始新世以来发生陆陆俯冲,印度板块的北东部首次开始碰撞缅甸板块。这次A型俯冲使得缅甸板块沿Sagaing走滑断裂向北继续漂移,最大的右行走滑位移达450 km。在Sagaing走滑断裂的控制下,睡宝盆地亦呈现2期构造特征:中新世,缅甸盆地内经历拉张和断裂,安德曼海(Andaman)打开,并且弧后扩张中心向南迁移,睡宝盆地即呈现拉张的构造环境;上新世—更新世,由于缅甸板块向北运动碰撞到亚洲板块的喜马拉雅断裂,受到阻挡,构造反转。睡宝盆地受挤压和扭压导致一系列的逆断层、花状构造,最终形成以南北向右行走滑为主、叠加东西向扭压的应力背景。 相似文献
5.
《地学前缘》2017,(4):341-351
全球汇聚板块边缘是产生8级以上大地震和破坏性海啸的地方,一直以来是全球科学家关注的焦点和热点区域。马尼拉俯冲带位于南海东部,也是许多地震、海啸和活火山活跃的区域。本文依据以往穿过马尼拉俯冲带的多条多道反射地震测线和海底地震仪剖面数据,分析了马尼拉俯冲带海沟沉积物充填厚度变化、增生楔宽度变化、海底变形特征以及地壳速度结构变化,提出马尼拉俯冲带具有明显的分段特征,分为北吕宋区段、海山链区段和南部西吕宋区段。不同区段的俯冲过程明显不同,提出俯冲增生和俯冲剥蚀(构造剥蚀)两种机制分别控制了该俯冲带的南、北区段。北段主要受到俯冲增生机制的控制,在海沟和弧前盆地之间形成巨大的增生楔构造,在南海北部大陆边缘10~15km厚的减薄陆壳不断俯冲作用下,引起许多与俯冲有关的地震活动和构造变形。南段海山链区段海底地形复杂和粗糙,在俯冲增生、剥蚀或构造剥蚀的联合控制下,5~6km厚大洋板块不断俯冲形成较小的增生楔结构,部分沉积物可能随着板块的俯冲被拖曳到板块边界的深部。 相似文献
6.
笔者系统分析了1918—2005年间中国大陆及其周缘发生的3130个中、强地震的震源机制解,根据其特征进行了岩石圈应力场构造分区,首次得到区域应力场的压应力轴和张应力轴空间分布的统计数字结果。在此基础上研究了应力场的区域特征、探讨了其动力学来源以及构造运动特征。总体结果表明,中国大陆及其周缘岩石圈应力场和构造运动可以归结为印度洋板块、太平洋板块、菲律宾海板块与欧亚板块之间相对运动,以及大陆板内区域块体之间的相互作用的结果。印度洋板块向欧亚板块的碰撞挤压运动所产生的强烈的挤压应力,控制了喜马拉雅、青藏高原、中国西部乃至延伸到天山及其以北的广大地区。在青藏高原周缘地区和中国西部的大范围内,压应力P轴水平分量方位位于20～40°,形成了近NE方向的挤压应力场。大量逆断层型强震集中发生在青藏高原的南、北和西部周缘地区,以及天山等地区。而多数正断层型地震集中发生在青藏高原中部高海拔的地区,断层位错的水平分量位于近东西方向。表明青藏高原周缘区域发生南北向强烈挤压短缩的同时,中部高海拔地区存在着明显的近东西向的扩张运动。中国东部的华北地区受到太平洋板块向欧亚板块俯冲挤压的同时,又受到从贝加尔湖经过大华北直到琉球海沟的广阔地域里存在着的统一的、方位为170°的引张应力场的控制。华北地区大地震的震源机制解均反映出该区地震的发生大体为NEE向挤压应力和NNW向张应力的共同作用结果。台湾纵谷断层是菲律宾海板块与欧亚板块之间碰撞挤压边界。来自北西向运动的菲律宾海板块构造应力控制了从台湾纵谷、华南块体,直到中国南北地震带南段东部地域的应力场。地震的震源机制结果还表明,将中国大陆分成东、西两部分的中国南北地震带是印度洋板块、菲律宾海板块与太平洋板块在中国大陆内部影响控制范围的分界线。 相似文献
7.
2014年于田Ms73地震地表破裂特征及其发震构造 总被引：2，自引：0，他引：2
2014年2月12日在新疆于田县境内西昆仑山东段地区发生了Ms7.3级强烈地震,震后野外考察表明,这次地震在海拔4600~5100m的地区形成了由一系列张裂隙、张剪裂隙、剪切裂隙以及挤压鼓包和裂陷等雁行状组合而成的地表破裂带,破裂带沿阿尔金断裂带西南段的两条近平行的分支断裂阿什库勒-硝尔库勒断裂和南硝尔库勒断裂分布,整体呈NEE走向,全长约28km,其中,沿阿什库勒-硝尔库勒断裂展布的地表破裂带长约10km,主要呈N63°~65°E走向,以左旋走滑伴随伸展性质的破裂为主,最大左旋位移约0.7m,最大垂直位移约0.4m;沿南硝尔库勒断裂展布的地表破裂带长约15km,呈N54°~60°E走向,以左旋走滑伴随逆冲性质的破裂为主,最大左旋位移约1m,最大垂直位移约0.75m;上述两破裂带之间沿N15°E方向由零星的张裂隙和右阶雁行状分布的张裂隙或张剪裂隙组成的不连续破裂带长约5km,显示为伸展具有左旋走滑的性质;另外,在南硝尔库勒断裂北侧沿N100°~110°E方向展布一系列具有挤压、右旋走滑性质的地表破裂带长约4km,宽约2km,与NEE走向的左旋走滑破裂带构成同震共轭破裂带。这种特殊的地表破裂样式是近期发生的强地震中结构最复杂的走滑断层型地表破裂。发震断裂属于阿尔金断裂带西南段尾端分支断裂,它与郭扎错断裂和龙木错断裂构成"阿尔金断裂"向SW方向的延伸部分,它们是青藏高原西部晚新生代强烈活动断裂,其大地震活动是由于印度和欧亚板块间碰撞而产生大陆变形的应变能释放过程。 相似文献
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苏拉威西岛北部属于马鲁古海板块,其主体是北苏拉威西海沟俯冲带与帕卢-科洛左旋走滑断裂所围限的岛北支和岛东支。大约5 Ma前,苏拉群岛沿Sorong断层与苏拉威西岛东支碰撞,导致北苏拉威西海沟俯冲后撤,引起了岛北支顺时针旋转约20°～25°,同时,西侧的帕卢-科洛断层发生了约4 cm/a的左旋走滑。本文利用综合地球物理方法,计算了该区三维温度、速度、黏性特征,认为：苏拉威西岛北部在左旋走滑、俯冲后撤过程中,地壳以脆性变形为主,但由于北苏拉威西海沟俯冲带在地壳内形成南向倾斜的软弱层,Moho面和地形“镜像”区域内形成脆、韧变形共存的组合。地幔变形为韧性变形,深度约100 km的上地幔低速流变层是地幔韧性变形的主控层位。在周边板块边界不断移动的动力学背景中,苏拉威西岛北部在地壳尺度以收缩-伸展变形为主,在岩石圈尺度以旋转变形为主。 相似文献
11.
Inversion of tsunami waveforms is a well-established technique for estimating the slip distributions of subduction zone earthquakes, with some of the most detailed results having been obtained for earthquakes in the Nankai Trough, SW Japan. The present study, although it uses a method and tsunami waveform data set almost identical to previous study, aims to improve on previous work by using a more precise specification of initial conditions for the calculation of tsunami Green's functions. Specifically, we incorporated four improvements in the present study: (1) we used a realistic plate model based only on seismic survey results, and assumed it to be the fault plane of the 1944 Tonankai earthquake; (2) the smallest subfaults consistent with the long wavelength approximation were used in the tsunami inversion analysis; (3) we included the effect of horizontal displacement of the ocean bottom on tsunami generation; and (4) we performed a checkerboard resolution test. As obtained in previous studies, a zone of high slip (> 2.0 m) was resolved off the Shima Peninsula. However, the more precise calculation of tsunami Green's functions has revealed additional detail that was not evident in previous studies, which we demonstrate is resolvable and correlates with the position of known faults in the accretionary prism. While there was little or no slip near the trench axis in the eastern part of the rupture zone, there was up to 1.5 m of slip resolved within 30 km of the trough axis in the western part, along the coast of the Kii Peninsula. This troughward slip zone coincides with the position of a large splay fault mapped in multichannel reflection surveys. Furthermore, it is also clear that the upper edge of the Enshu fault off Shima and Atsumi peninsulas is consistent with the up-dip limit of slip in the eastern part of our model. We tested the possibility that slip occurred on the former splay fault instead of on the plate interface during the 1944 Tonankai earthquake, and find that slip on this splay fault is also consistent with the data, although we cannot distinguish whether slip was dominant on the splay fault or on the plate interface. We further suggest that the position of the Enshu fault may be determined by the subduction of topographic highs, and that such faults may have an important influence on the up-dip rupture limit of the 1944 Tonankai and, potentially, other subduction zone earthquakes. 相似文献
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The 2011 Tohoku earthquake and tsunami motivated an analysis of the potential for great tsunamis in Hawai‘i that significantly exceed the historical record. The largest potential tsunamis that may impact the state from distant, Mw 9 earthquakes—as forecast by two independent tsunami models—originate in the Eastern Aleutian Islands. This analysis is the basis for creating an extreme tsunami evacuation zone, updating prior zones based only on historical tsunami inundation. We first validate the methodology by corroborating that the largest historical tsunami in 1946 is consistent with the seismologically determined earthquake source and observed historical tsunami amplitudes in Hawai‘i. Using prior source characteristics of Mw 9 earthquakes (fault area, slip, and distribution), we analyze parametrically the range of Aleutian–Alaska earthquake sources that produce the most extreme tsunami events in Hawai‘i. Key findings include: (1) An Mw 8.6 ± 0.1 1946 Aleutian earthquake source fits Hawai‘i tsunami run-up/inundation observations, (2) for the 40 scenarios considered here, maximal tsunami inundations everywhere in the Hawaiian Islands cannot be generated by a single large earthquake, (3) depending on location, the largest inundations may occur for either earthquakes with the largest slip at the trench, or those with broad faulting over an extended area, (4) these extremes are shown to correlate with the frequency content (wavelength) of the tsunami, (5) highly variable slip along the fault strike has only a minor influence on inundation at these tele-tsunami distances, and (6) for a given maximum average fault slip, increasing the fault area does not generally produce greater run-up, as the additional wave energy enhances longer wavelengths, with a modest effect on inundation. 相似文献
13.
Aftab Alam Khan 《Natural Hazards》2012,61(3):1127-1141
Geodynamic status, seismo-tectonic environment, and geophysical signatures of the Bay of Bengal do not support the occurrence
of seismogenic tsunami. Since thrust fault and its intensity and magnitude of rupture are the key tectonic elements of tsunamigenic
seismic sources, the study reveals that such characteristics of fault-rupture and seismic sources do not occur in most of
the Bay of Bengal except a small segment in the Andaman–Nicobar subduction zone. The inferred segment of the Andaman–Nicobar
subduction zone is considered for generating a model of the deformation field arising from fluid-driven source. The model
suggests local tsunami with insignificant inundation potential along the coast of northern Bay of Bengal. The bathymetric
profile and the sea floor configuration of the northern Bay of Bengal play an important role in flattening the waveform through
defocusing process. The direction of motion of the Indian plate makes an angle of about 30° with the direction of the opening
of Andaman Sea. The opening of Andaman Sea and the direction of plate motion of the Indian plate results in the formation
of Andaman trench where the subducting plate dives more obliquely than that in the Sunda trench in the south. The oblique
subduction reduces significantly the possibilities of dominant thrust faulting in the Andaman subduction zone. Further, north
of Andaman subduction in the Bengal–Arakan coast, there is no active subduction. On the otherhand, much greater volume of
sediments (in excess of 20 km) in the Bengal–Arakan segment reduces the possibilities of mega rupture of the ocean floor.
The water depth (≈1,000 m) along most of the northern Bay of Bengal plate margin is not optimum for any significant tsunami
generation. Hence, very weak possibility of any significant tsunami is suggested that based on the interpretation of geodynamic
status, seismo-tectonic environment, and geophysical signatures of the Andaman subduction zone and the Bengal–Arakan coast. 相似文献
14.
Oblique subduction at the Sunda Trench has produced transpressive deformation of the plate leading edge. A major feature is the right-lateral Great Sumatran Fault (GSF) which probably absorbs a significant fraction of the trench-parallel shear. The kinematics of Sunda relative to Australia are discussed on the basis of available GPS data, and geologically determined slip rates on the GSF. In spite of the uncertainty on the plate motion, several robust conclusions can be drawn. The predicted obliquity of the convergence increases northward along the Sumatra Trench, up to about 30°. Slip partitioning is nearly complete along the northern segment of the Sumatra Trench, where the GSF probably accommodates most of the trench parallel shear. Along the southern segment, where obliquity is less than about 20°, slip-partitioning is not complete as indicated by oblique thrusting at the subduction. There, only a fraction of the trench parallel motion of Australia relative to SE Asia is accommodated along the GSF. These observations suggest that the leading edge behaves like a plastic wedge, except that slip-partitioning, although incomplete, is observed even at low obliquities. 相似文献
15.
P. Mahesh Amit Bansal B. Kundu J. K. Catherine V. K. Gahalaut 《Journal of the Geological Society of India》2011,77(3):243-251
The recent 10 August 2009 Coco earthquake (Mw 7.5), the largest aftershock of the giant 2004 Sumatra Andaman earthquake, occurred
within the subducting India plate under the Burma plate. The Coco earthquake nucleated near the northwestern edge of the 2004
Sumatra-Andaman earthquake rupture under the unruptured updip segment of the plate boundary interface. The earthquake with
predominant normal motion on approximately north-south to northeast-southwest oriented plane is very similar to the 27 June
2008 Little Andaman earthquake which occurred in the South Andaman region near the trench. We provide the only available estimate
of coseismic offset due to the 2009 Coco earthquake at a survey-mode GPS site in the north Andaman, located about 60 km south
of the Coco earthquake epicentre. The not so large coseismic displacement of about 2 cm in the ESE direction is consistent
with the earthquake focal mechanism and its magnitude. We suggest that, like the 2008 Little Andaman earthquake, this earthquake
too occurred on one of the approximately north-south to northeast-southwest oriented steep planes of the obliquely subducting
90°E ridge which was reactivated in normal motion after subduction, under the favourable influence of coseismic and ongoing
postseismic deformation due to the 2004 Sumatra-Andaman earthquake. Another notable feature of this earthquake is its relatively
low aftershock productivity. We suggest that the earthquake occurred very close to the aseismic region of the Irrawaddy frontal
arc of very low seismicity where pre-existing faults are not so critically stressed and because of which the earthquake could
trigger only a few aftershocks in its immediate vicinity. 相似文献
16.
Laishram Sunil Singh V. K. Gahalaut Arun Kumar 《Journal of the Geological Society of India》2014,83(5):513-516
We report results of 9 years of GPS measurements of crustal deformation at Imphal, Manipur, a site located in the Indo-Burmese wedge of northwest Sunda arc. The analysis of these measurements suggests that the site moves at a rate of about 36.3±0.5 mm/year towards N55° in the ITRF2008. With respect to the Indian plate it moves at a rate of 16.7 mm/year towards N222°, i.e., predominantly towards southwest. The site is located about 15 km east of the Churachandpur Mao fault (CMF), which is reported to accommodate part of the India-Sunda motion. The site motion is not significantly affected by the earthquakes that occurred in the nearby region. However, the 2004 Sumatra-Andaman earthquake caused a coseismic displacement of ～ 3–5 mm predominantly towards southwest. The site motion is almost linear, with some seasonal variation, and does not show any evidence of accelerated slip or slow earthquake on the CMF or along the plate boundary. 相似文献
17.
HarshGupta 《《幕》》2005,28(1):2-5
The 26th December 2004 earthquake of Mw 9.3 is the second largest earthquake ever to have been recorded.This generated a tsunami which affected several Asian countries. In India, the Andaman & Nicobar group of islands, and coastal states of Tamil Nadu, Andhra Pradesh and Kerala were severely affected. Here, we briefly provide an outline of the approach taken by India for an early warning system for mitigation of oceanogenic disasters. 相似文献
18.
2022年1月8日青海门源MS 6.9地震发生在青藏高原东北缘的祁连山断块内部,仪器震中位于海原活动断裂系西段的冷龙岭断裂带上,是该断裂系自1920年海原8.5级大地震后再次发生M>6.5的强震。考察结果的初步总结表明,此次门源地震产生了呈左阶斜列分布、总长度近23 km的南北两条破裂,在两者之间存在长约3.2 km、宽近2 km的地表破裂空区。南支破裂(F1)出现在托来山断裂的东段,走向91°,长约2.4 km,以兼具向南逆冲的左旋走滑变形为主,最大走滑位移近0.4 m。北支主破裂(F2)出现在冷龙岭断裂的西段,总长度近20 km,以左旋走滑变形为主,呈整体微凸向北东的弧形展布,包含了走向分别为102°、109°和118°的西、中、东三段,最大走滑位移出现在中段,为3.0±0.2 m。此外,在北支主破裂中—东段的北侧新发现一条累计长度约7.6 km、以右旋正断为主的北支次级破裂(F3),累计最大走滑量约0.8 m,最大正断位移约1.5 m。综合分析认为,整个同震破裂以左旋走滑变形为主,具有双侧破裂特点,宏观震中位于北支主破裂的中段,其地表走滑位移很大可能与震源破裂深度浅有关,其中的右旋正断次级破裂可能是南侧主动盘向东运移过程中拖曳北侧块体发生差异运动所引起的特殊变形现象。印度与欧亚板块近南北向强烈碰撞挤压导致南祁连断块沿海原左旋走滑断裂系向东挤出,从而引发该断裂系中的托来山断裂与冷龙岭断裂同时发生破裂,成为导致此次强震的主要动力机制。在此大陆动力学背景下,以海原左旋走滑断裂系为主边界的祁连山断块及其周边的未来强震危险性需得到进一步重视。 相似文献
19.
Genesis of a new slab tear fault in the Indo-Australian plate,offshore northern Sumatra,Indian ocean
Following the December 2004 and March 2005 major shallow foci inter-plate earthquakes in the north Sumatra region, a slab-tear fault located within the subducting Indian plate ruptured across the West Sunda Trench (WST) within the marginal intra-plate region. Trend, length and movement pattern of this New Tear Fault (NTF) segment is almost identical to another such slab-tear fault mapped previously by Hamilton (1979), located around 160 km south of NTF. Seismic activity along the NTF remained quasi-stable till the end of the year 2011, when an earthquake of magnitude 7.2 occurred on 10.01.2012 just at the tip of NTF, only around ～100 km within the intra-plate domain west of WST. The NTF rupture propagated further towards SSW with the generation of two more large earthquakes on 11.04.2012. The foreshock (10.01.12; M7.2) — mainshock (11.04.12; M 8.6) — aftershock (11.04.12; M 8.2) sequence along with numerous smaller magnitude aftershocks unmistakably define the extension of NTF, a slab-tear fault that results tectonic segmentation of the convergent plate margin. Within the intra-plate domain most earthquakes display consistent left-lateral strike slip mechanism along NNE trending fault plane. 相似文献