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2018年9月8日,云南省墨江县发生MS5.9地震并伴随一系列余震,探究该地震周围的应力场对于理解该地震的发生机制和后续地震的发展趋势具有着重要的参考意义.本研究收集了震源及其邻区中前人研究和Global CMT所给出的震源机制资料,对该地区进行了构造应力场反演,并同时利用反演得到的应力张量模拟墨江地区的震源机制解表现.结果表明:(1)在应力轴整体分布上,自西向东σ1轴(压轴)从NNE-SSW向逐渐转向NNW-SSE向,σ3轴(张轴)从WWN-EES向逐渐转向WWS-EEN向,张轴呈弧形分布,压轴呈放射状分布.(2)在应力轴倾伏角上,研究区域内的压应力轴和张应力轴倾伏角都比较小,即两轴均接近水平.(3)R值分布大体是在东南部相较于西北部大,结合当地地质背景分析得到,物质逃逸自西北向东南呈逐渐变缓的趋势.(4)利用反演得到的应力张量和应力状态计算墨江地震震源区的相对剪应力和相对正应力大小.由此推测,墨江地震恰好发生在相对剪切应力值和相对正应力正值最大的节面上.从而可以确定墨江地震的发震节面的基本参数:走向216.32°,倾角86.91°,滑动角0.27°,相对剪应力值0.9,相对正应力值0.3.本研究为此次墨江地震的发震背景和地震动力学研究提供了基础性资料. 相似文献
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2011年腾冲地区连续发生了3次中强地震,本文运用全波形模拟的方法研究了这3次中强地震序列的震源机制解,并对地震序列进行了重定位。笔者结合由震源机制解及重定位结果对其发震构造进行了分析,认为3次中强地震及序列均位于同一发震构造,呈北西走向,破裂面倾角陡直,在近水平的北北东向压应力作用下作右旋水平走滑错动,断层较浅仅限于上地壳,活动过程有向深部发展的趋势;震源区附近无明显已知构造与发震构造相对应,发震构造可能为未知隐伏构造。 相似文献
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The principal stress axes and eigenvalue ratios of the stress tensors from two active seismic regions in Alaska (eastern Aleutian Arc and eastern Gulf of Alaska) are computed. These results are obtained using focal mechanisms of earthquakes with magnitudes ranging from 5.5 to 8.2 and show for both regions slightly different compressional states with an orientation of the pressure axis of N26°W for the eastern Gulf of Alaska and N27°W for the east Aleutian Arc. The eigenvalue ratios for the eastern Gulf of Alaska and east Aleutian Arc are 0.84 and 0.99, respectively. The algorithm used in computations allows us to detect some focal mechanisms which are incoherent with respect to the obtained stress tensors. These incoherences are explained in terms of some tectonic features of the region. The orientations of possible pre-existing fractures which would need an unrealistically high maximum shear stress to start a slip on their fault planes are also investigated. These critical orientations depend on a constitutive frictional law as well as on eigenvalue ratios and eigenvectors of the stress tensors. The orientation, which is given in our case by the angle between the normal vector to a fracture and the regional tensional axis, is approximately 59° for the eastern Aleutian Arc. This angle ranges from 49° to 59° for the eastern Gulf of Alaska. It must be pointed out that fractures which need unrealistically high shear stress to start slip on their fault planes are defined by a very narrow band of possible angles between tensional direction and the normal vector to fault plane. 相似文献
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地震主应力方向的附加潮汐应力计算及其对发震断层的作用方式研究 总被引：4，自引：0，他引：4
通过对地震震源处沿主压应力P轴和主张应力T轴方向的附加潮汐应力分量的计算，在岩石力学莫尔－库化准则的基础上分析了附加潮汐应力对发震断层的作用方式。分析和计算表明，对发震断层有促滑作用的附加潮汐应力作用方式分增压型和减压型，增压型潮汐应力增大断层面上的正压力和剪应力，促使断层达到破裂滑动条件，减压型潮汐应力在一定条件下能降低断层面上的破裂滑动强度，同样能促使断层的运动。计算实例显示，大部分发震断层受到了附加潮汐应力的增压型或减压型促滑作用。 相似文献
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2017年8月9日新疆精河发生MS6.6地震,深入了解该地震的构造应力背景及其所破裂断层的活动特性对理解其孕震过程及震后的地震危险性估计十分重要.本研究自GCMT目录收集了2017年8月9日新疆精河MS6.6地震震中及其邻区的253个震源机制解,应用MSATSI软件反演了该地震及其邻区的应力场.反演结果显示,西北区域应力场的最大主压应力轴的方位从西到东呈现出NNW-NS-NNE的渐变过程,东南区域应力场最大主压应力轴的方位稳定于NNE向,倾角都较小;最大主张应力轴都基本沿东西向,倾角相对较大;西北区域较大的R值显示出区域应力场主要受近NS向水平挤压作用,中部挤压分量相对较大,西部和东部挤压分量相对较小.根据所反演的区域构造应力场,结合发震的库松木契克山前断裂的地质调查参数,估算该断裂的理论滑动角为137.7°,误差为21.3°,验证了地质上得到的库松木契克山前断裂的逆冲兼右旋走滑性质.判断该断裂滑动性质的另一种方法是通过发生在该断裂上地震的震源机制验证.本研究首先计算了发生在库松木契克山前断裂不同机构给出的震源机制节面在所反演的局部应力场作用下的理论滑动角,发现理论滑动角与实际地震震源机制滑动角相差很小,验证了反演的局部应力场的正确性;而后计算了局部应力场作用下的库松木契克山前断裂上的理论震源机制与实际发生地震震源机制的三维空间旋转角,发现两者在给定的误差范围内是一致的.本研究自地球物理角度确证了库松木契克山前断裂的滑动性质,为该地区的地震孕育环境、地震活动性和地球动力学研究提供了基础. 相似文献
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中国西部强震构造的初步研究 总被引：1，自引：0，他引：1
以地震破裂带,极震区长轴及发震断裂等为基础资料,统计了中国西部的强震构造。结果表明,其走向和长度均服从正态分布,并存在线性相关关系。为此,建立了构造走向与长度之间的回归方程。分析了破裂带与地震构造类型、发霉构造与区域应力场之间的关系,讨论了北西向发震构造在中国西部占主导地位的原因。 相似文献
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使用唐山地区2002年1月—2015年11月ML≥2.5地震的255个震源机制解, 采用构造应力场均匀性的分段方法对唐山地震序列的发震断层进行分段． 在已有唐山地区震源机制解分区特征的基础上, 给出了5个参考应力张量, 并通过差异显著性的z值检验计算将唐山地震序列的发震断层分为宁河、 唐山、 滦县和卢龙等4个子段, 进而分别对4个子段的应力场进行反演． 结果显示: 4个子段的最大主压应力方向均呈近EW向, 且唐山、 宁河和卢龙子段的应力场均表现出较大的拉张分量; 唐山、 宁河子段的最佳应力张量与唐山主震对唐山断裂带两端点所产生的引张应力场的作用方式一致． 此外, 唐山子段的应力场符合基于接收函数给出的上地幔物质隆升模型, 滦县子段走滑型的应力状态反映了该区的共轭构造运动, 卢龙子段的最佳应力张量为正断兼右旋走滑． 从当前唐山地震序列发震断层分段的应力场特征可以推断, 现今唐山地区的地震活动具有继承性, 主要受区域构造应力场和该区深、 浅共存的断裂构造体系控制． 相似文献
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Variations in stress and driving pore fluid pressure ratio using vein orientations along megasplay faults : Example from the Nobeoka Thrust,Southwest Japan 
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下载免费PDF全文 Makoto Otsubo Ayumu Miyakawa Ryoji Kawasaki Katsushi Sato Asuka Yamaguchi Gaku Kimura 《Island Arc》2016,25(6):421-432
The Nobeoka Thrust of Southwest Japan is an on‐land example of an ancient megasplay fault that provides an excellent record of deformation and fluid flow at seismogenic depths. The present study reports: (i) temporal stress changes for the seismogenic period of the Nobeoka Thrust; and (ii) spatial heterogeneities in driving pressure ratios P* obtained from mineral veins around the Nobeoka Thrust fault zone. Many quartz veins that filled mode I cracks can be observed in the hanging wall and footwall of the thrust. Inversion for stress orientation suggests that normal faulting dominated in both the hanging wall and footwall, with similar stress axis orientations in both. The orientation of σ3 for the estimated stress regime is parallel to the slip direction of the Nobeoka Thrust. The detected normal‐faulting‐type stress regimes likely resulted from post‐seismic stress buildup after megathrust earthquakes. The hanging wall of the Nobeoka Thrust has smaller P* values than the footwall. Two possible explanations are proposed for the observed spatial variations in the driving pore fluid pressure ratio, P*: spatial variations in pore fluid pressure Pf are directly responsible for P* variations, or P* variations are controlled by differences in mechanical properties between the hanging wall and footwall. 相似文献
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美国哈佛大学1977——2004年的矩心矩张量结果显示, 我国川西北次级地块、 滇中次级地块的西部及滇中次级地块的东部的应力场特征有明显的差别. 应用滑动矢量拟合法, 反演了这三个区域的应力场特征: 川西北次级地块以近南北向的水平主张应力轴和西倾的主压应力轴为特征; 滇中次级地块的西部以倾向北东东的主张应力轴以及近南北的水平中等主应力轴为特征; 滇中次级地块的东部以南西西——北东东向的水平主张应力轴以及北北西——南南东向的水平主压应力轴为特征. 有限元模拟结果清楚地显示出, 川滇地块在阿萨姆楔附近受到来自印度板块的强烈挤压, 随着远离阿萨姆楔, 这种挤压应力逐渐衰减; 同时, 该地区的主张应力方向明显地形成了围绕阿萨姆楔的环线. 其中, 内部物质性质均匀、 地表和底部边界自由、 侧部边界采用GPS观测约束的弹性有限元模拟显示, 在川西北次级地块, 模拟结果与震源机制解结果相一致; 在滇中次级地块, 模拟结果所显示的图象与震源机制解观测结果有差别, 不仅没有显示出与大面积的东部地区的震源机制解相一致的特征, 反而显示出与该地区西部震源机制解相一致的特征. 通过调节地块内部物质的弹性常数, 可以实现在滇中次级地块东部部分地区出现与震源机制 相似文献
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本文选取辽宁海城、 盖州地区(40°~41°N, 122°~123°E)作为研究区, 利用广义极性振幅技术(GPAT)方法, 反演得到研究区2012—2017年6月共184个地震震源机制解, 并利用Misfit角度分析震源机制一致性参数特征。 研究结果表明: ① 研究区地震震源机制解以走滑型和正断型为主。 海城地区地震震源机制解以NW—SE向节面的左旋走滑型和NWW向节面的正断型为主。 发震构造以NW向海城河断裂为主, NE向节面为主的地震可能受到NE向金州断裂带的控制。 ② 青石岭地区的发震构造为与九寨—盖县北段共轭的NW向未知断裂, 西海域的地震活动可能是NE向的雁式断裂和NW向共轭的未知断裂共同作用的结果。 ③ 震源机制一致性结果显示, 一致性增强后发生了震级相对较大的地震。 研究区的震源机制一致性较强, 表明该区域的应力较为集中。 但由于2016年以来活动趋于平静, 尚难以根据震源机制解一致性程度做出当前应力状态的判断。 相似文献
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采用构造应力场均匀性对断层或板块边界进行分段的方法, 利用ldquo;裁剪-粘贴rdquo;法给出的余震震源机制解资料, 进一步从应力场角度确定汶川地震发震断层南、 北段分界点位置及南、北段震后应力场. 研究结果表明, 发震断层南、北段分界点位于北川附近, 与先前的研究结果较为一致. 南、 北段震后应力场反演结果显示, 南、北段的最大主应力轴方位均呈北东东向, 且近水平. 南、北段应力场反演的平均拟合残差和置信区间均较大, 主要原因可能是因为南、北段内应力场不均匀性造成的. 因为本文仅由大余震给出了震源断层的一级分段, 南、北段内应做进一步的细分. 相似文献
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In this paper we discuss the seismogenic process of a great earthquake by using a rheologic model of rock. We regard the constant strain rate as the condition of seismogeny for a great earthquake. On the basis of analytic results, the curves of variation of stress, strain, strain rate and energy with time are calculated. Upon such curves, the stage features of the seismogenic process of a great earthquake is analyzed. And the possible mechanisms of the various seismic precursory phenomena is emphatically discussed, and the relation between the preseismic anomalous phenomena and the seismogenic process is given. 相似文献
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不同资料和方法给出的2019年6月17日四川长宁6.0级地震震源机制解存在较大差异,为了找到1个合适的震源机制解来研究此次地震的发震方式,通过数学方法得到了与现有震源机制解差别最小的中心震源机制解,节面I的走向、倾角、滑动角分别为194.78°、52.68°和139.16°,节面Ⅱ的走向、倾角、滑动角分别为312.44°、58.67°和45.22°,根据本次地震余震分布拟合得到的断层面的走向为312.17°,与中心震源机制的节面Ⅱ走向一致,因而推断节面Ⅱ为本次地震的发震断层面。之后,利用此次地震之前震源区地震的震源机制解,反演了震源区的震前构造应力场。结果表明,长宁6.0级地震的中心震源机制解和震源区震前应力场均为逆冲型为主兼走滑分量的类型,震前应力场压轴为NWW—SEE向,中间轴为NNE—SSW向,两轴倾角接近水平,而张轴较陡,表现为逆冲型的应力场。将反演得到的应力场投影到中心震源机制解给出的与余震分布一致的节面上,发现中心震源机制解的滑动角和应力场预测的滑动角差别仅为13.45°,表明此次地震受背景应力场控制而发生在先存的薄弱面上。 相似文献
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于2011年3月11日发生在日本东北部的MW9.0级逆冲型板间地震是日本有地震记录以来震级最大的一次地震.本研究基于NIED F-net矩张量解目录中的震源机制解,选取两个长轴相互垂直的矩形区域进行应力场2D反演,获取了日本海沟俯冲带地区应力场的空间及时间分布图像.结果表明：主震前,俯冲带地区应力状态在空间上大体趋于一致,即应力轴（P轴、σ1轴及SHmax轴）系统性地倾向板块汇聚方向,P轴、σ1轴倾角整体偏缓（<30°）,且远离震源区及日本海沟东侧区域内的应力轴倾角普遍大于主震震源区内应力轴倾角;主震前,受2003年5月26日在宫城县北部发生的MW7.0地震影响,位于MW9.0地震震源区西北侧的应力场出现明显扰动,σ1轴倾向顺时针偏转150°~180°,并于之后大体恢复至震前状态,同期其他地区没有明显变化,这种情况可能和主震断层局部（深部）的前兆性滑动有关;主震后,距离震源区较远处应力场变化不大,主震震源区内应力场发生显著改变,P轴及σ1轴均以大角度（>60°）倾伏于板块汇聚方向,SHmax轴顺时针偏转60°~90°且在日本海沟附近普遍平行于海沟轴.这项研究以时空图像的方式展示了大地震前应力场变化的特点,反映了大地震孕震过程中构造与地震的相互作用,对于理解大地震孕震过程有重要意义. 相似文献
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STUDY ON THE SEISMOGENIC FAULT AND DYNAMICS PARAME-TERS OF THE 2014 MS6.6 JINGGU EARTHQUAKE IN YUNNAN 下载免费PDF全文
下载免费PDF全文 On October 17, 2014, a MS6.6 earthquake occurred in Jinggu, Yunnan. The epicenter was located in the western branch of Wuliang Mountain, the northwest extension line of Puwen Fault. There are 2 faults in the surrounding area, one is a sinistral strike-slip and the other is the dextral. Two faults have mutual intersection with conjugate joints property to form a checkerboard faulting structure. The structure of the area of the focal region is complex. The present-day tectonic movement is strong, and the aftershock distribution indicates the faulting surface trending NNW. There is no obvious surface rupture related to the known fault in the epicenter, and there is a certain distance from the surface of the Puwen fault zone. Regional seismic activity is strong. In 1941, there were two over magnitude 7.0 earthquakes in the south of the epicenter of Jinggu County and Mengzhe Town. In 1988, two mainshock-aftershock type earthquakes occurred in Canglan-Gengma Counties, the principal stress axes of the whole seismic area is in the direction of NNE. Geological method can be adopted to clarify the distribution of surficial fracture caused by active faults, and high-precision seismic positioning and spatial distribution characteristics of seismic sequences can contribute to understand deep seismogenic faults and geometric features. Thus, we can better analyze the three-dimensional spatial distribution characteristics of seismotectonics and the deep and shallow tectonic relationship. The focal mechanism reveals the property and faulting process to a certain extent, which can help us understand not only the active property of faults, but also the important basis for deep tectonic stress and seismogenic mechanism. In order to study the fault characteristic of the Jinggu earthquake, the stress field characteristics of the source area and the geometric parameters of the fault plane, this paper firstly uses the 15 days aftershock data of the Jingsuo MS6.6 earthquake, to precisely locate the main shock and aftershock sequences using double-difference location method. The results show that the aftershock sequences have clustering characteristics along the NW direction, with a depth mainly of 5~15km. Based on the precise location, calculations are made to the focal mechanisms of a total of 46 earthquakes including the main shock and aftershocks with ML ≥ 3.0 of the Jinggu earthquake. The double-couple(DC)component of the focal mechanism of the main shock shows that nodal plane Ⅰ:The strike is 239°, the dip 81°, and the rake -22°; nodal plane Ⅱ, the strike is 333°, the dip 68°, and the rake -170.31°. According to focal mechanism solutions, there are 42 earthquakes with a focal mechanism of strike-slip type, accounting for 91.3%. According to the distribution of the aftershock sequence, it can be inferred that the nodal plane Ⅱ is the seismogenic fault. The obtained focal mechanism is used to invert the stress field in the source region. The distribution of horizontal maximum principal stress orienation is concentrated. The main features of the regional tectonic stress field are under the NNE-SSW compression(P axis)and the NW-SE extension(T axis)and are also affected by NNW direction stress fields in the central region of Yunnan, which indicates that Jinggu earthquake fault, like Gengma earthquake, is a new NW-trending fault which is under domination of large-scale tectonic stress and effected by local tectonic stress environment. In order to define more accurately the occurrence of the fault plane of the Jinggu earthquake, with the precise location results and the stress field in the source region, the global optimal solution of the fault plane parameters and its error are obtained by using both global searching simulated annealing algorithm and local searching Gauss-Newton method. Since the parameters of the fault plane fitting process use the stress parameters obtained by the focal mechanism inversion, the data obtained by the fault plane fitting is more representative of the rupture plane, that is, the strike 332.75°, the dip 89.53°, and the rake -167.12°. The buried depth of the rupture plane is 2.746km, indicating that the source fault has not cut through the surface. Based on the stress field characteristics and the inversion results of the fault plane, it is preliminarily believed that the seismogenic structure of the Jinggu earthquake is a newly generated nearly vertical right-lateral strike-slip fault with normal component. The rupture plane length is about 17.2km, which does not extend to the Puwen fault zone. Jinggu earthquake occurred in Simao-Puer seismic region in the south of Sichuan-Yunnan plate. Its focal mechanism solution is similar to that of the three sub-events of the Gengma earthquake in November 1988. The seismogenic structure of both of them is NW-trending and the principal stress is NE-SW. The rupture plane of the Jinggu main shock(NW direction)is significantly different from the known near NS direction Lancang Fault and the near NE direction Jinggu Fault in the study area. It is preliminarily inferred that the seismogenic structure of this earthquake has a neogenetic feature. 相似文献
19.
Investigation of Coulomb stress changes in south Tibet(central Himalayas) due to the 25th April 2015 M_W 7.8 Nepal earthquake using a Coulomb stress transfer model 下载免费PDF全文
下载免费PDF全文 After M_W 7.8 Nepal earthquake occurred, the rearrangement of stresses in the crust commonly leads to subsequent damaging earthquakes. We present the calculations of the coseismic stress changes that resulted from the 25 th April event using models of regional faults designed according to south Tibet-Nepal structure, and show that some indicative significant stress increases. We calculate static stress changes caused by the displacement of a fault on which dislocations happen and an earthquake occurs. A M_W 7.3 earthquake broke on 12 May at a distance of * 130 km SEE of the M_W 7.8 earthquake, whose focus roughly located on high Coulomb stress change(CSC) site. Aftershocks(first 15 days after the mainshock)are associated with stress increase zone caused by the main rupture. We set receiver faults with specified strikes, dips,and rakes, on which the stresses imparted by the source fault are resolved. Four group normal faults to the north of the Nepal earthquake seismogenic fault were set as receiver faults and variant results followed. We provide a discussion on Coulomb stress transfer for the seismogenic fault, which is useful to identify potential future rupture zones. 相似文献
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本文首先利用加卸载响应比孕震积分, 对2001年以来新疆境内南天山西段和喀什—乌恰交汇区发生的4次MS≥6.0地震, 进行了震例检验。 结果显示, 孕震初期孕震积分在背景值附近波动, 变化平缓。 随着孕震程度的加剧, 孕震积分不断增加至峰值点, 快速回落过程中或恢复后发震。 我们还将加卸载响应比孕震积分初步应用到南天山西段的部分定点形变资料中, 对比分析了哈拉峻台、 乌恰台钻孔倾斜以及乌什水管仪、 伸缩仪和体应变趋势日均值与以台站为中心, 250 km为半径的加卸载响应比孕震积分时序图。 结果表明, ① 哈拉峻台和乌恰台区域内构造应力场应力处于不断加载的过程, 引起了定点形变资料速率的大幅度、 不稳定变化; ② 当构造应力场上的应力处于缓慢不断加载的过程时, 会引起定点形变测项速率方向发生改变, 表现形式为趋势异常; ③ 目前, 南天山西段构造应力场应力水平处于不断加载的过程。 相似文献