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四川3次7级以上地震序列和余震分布特征的对比 总被引：1，自引：0，他引：1
本文对比了汶川8．0级、炉霍7．6级和松潘、平武7．2级地震的地震序列类型、余震分布形状及其阶段性特征,并分析了这些特征异同与发震断裂带的特性关系。主要结论有：（1）扩大川滇其他震例对比统计认为,位于活动地块边界的大型活动断裂带上的强震往往是主震—余震型,双震或震群型地震往往不在块体边界大断裂带上。（2）强震余震区形状和余震随时间分布的阶段性受发震断裂带组合方式制约。 相似文献
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以 2 0 0 1年 11月 14日昆仑山 8 1级地震为例 ,运用月均亮温点对点差值分析法和断裂带内外亮温差值分析法 ,研究了活动断裂与震前红外异常的空间关系及发震断裂上震前卫星红外异常的时间演化过程。研究发现 :震前月平均亮温相对于 2 0 0 0年同期平均亮温的增温区沿发震断裂呈条带状分布 ;从震前 1个半月的 2 0 0 1年 10月开始 ,断裂带内外的相对温差发生明显变化 ,断裂带内的平均亮温与其外围的平均亮温差从 - 2℃增加到 1℃ ,相对增温幅度达 2～ 3℃左右 ,地震之后相对温差又回到正常状态。由此可见 ,震前卫星红外增温与东昆仑断裂带存在着明显的对应关系 ;地震前沿断裂带的红外增温大于其它地区。断裂带内外亮温差值分析法是定量研究红外增温与活动断裂的时空关系、挖掘震前增温异常的有效方法 相似文献
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我国东北地区地震时空演变特征及其动力学研究 总被引：5，自引：0，他引：5
本文分析了我国东北地区中强地震空间分布特征和地震构造及震源机制特点,探讨了日本海俯冲带大地震迁移方向对中国东北地区中强地震空间分布的影响。结果表明:东北地区中强地震发震构造以NW向为主,Ms≥5 0的地震NW向发震构造约占67%,Ms≥5 8的地震NW向发震构造约占91%;日本海俯冲带大地震迁移方向对中国东北地区浅震的空间分布产生重要影响,当迁移方向与郯庐断裂带夹角较大时(α≥70°),地震主要发生在松辽盆地及其周边;当迁移方向与郯庐断裂带夹角较小时(α<70°),地震主要发生在郯庐断裂带附近。 相似文献
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汶川地震同震形变场对川滇地区主要活动断裂地震发生趋势的影响 总被引：5，自引：0，他引：5
以所建立的川滇地区主要活动块体及其周边断裂带的模型和前期利用GPS及水准资料反演所得到的断裂带长期运动速率作为基础,将汶川地震引起的同震错动量加入到三维断裂几何模型中,计算出汶川地震大范围的同震形变场,然后基于该同震形变场和活动断裂三维几何模型反演了各条断裂对该同震形变场的反映,并通过与各断裂带长期运动速率对比,得到了汶川地震对川滇地区各主要活动断裂带发震趋势的影响．结果表明,在汶川地震引起的同震形变场作用下,在川滇交界东部地区,龙门山断裂带南西段地震危险性提前了305a,鲜水河断裂带南东段大致提前了19a,安宁河断裂带和则木河断裂带分别提前了21a和12a,大凉山断裂带北段和南段分别提前了9.1a和18a,马边断裂带的地震危险性则提前了51a;对川滇交界西部的丽江——小金河断裂带南西段、怒江断裂带、龙陵——澜沧断裂带、南汀河断裂带、中甸断裂带等断裂带地震的能量积累也有促进作用;相反在鲜水河断裂带北西段、小江断裂带等历史地震频发的断裂带上,地震危险性具有一定的减速作用． 相似文献
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地震序列的特征和震型判定工作有助于抗震救灾工作的开展,对其发生成因的研究是解决地震预报难题必须面对的科学问题。汶川8．0级地震序列的初步研究表明：①余震沿龙门山断裂带分布于宽100km,长约330km的带状区域内,并侧向于主震震中的北侧;②序列发展初期有2个快速衰减过程;③序列类型为主震一余震型,最大强余震6．4级;④序列的空间演化过程,强余震震源机制结果和地震精确定位结果分析表明,序列具有分段特征;⑤8．0级地震的发震构造是龙门山断裂带,发震构造在剖面上呈现出“犁形”或“铲形”。地球物理勘探和壳、幔结构反演结果表明,自青藏高原穿越龙门山到四川盆地存在地幔阶梯,上地幔阶梯的阻挡作用使得物质东移速率减慢,并蕴积了汶川8．0级地震所需能量。地震的产生正是东西向应力平衡被打破的结果,余震沿龙门山断裂的分布是高原地壳在印度板块的推挤作用下向北北东方向的运动得以继续的表现。整个龙门山断裂带都参与了活动,龙门山断裂带北端作为断裂带的止裂端与南段同期活动。 相似文献
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福建政和-海丰断裂带地震活动特征分析 总被引：1，自引：0，他引：1
通过对1971年以来福建政和-海丰断裂带地震活动特征分析后认为：北东向的政和-海丰断裂带和次一级北西向的永安-晋江断裂带相互交汇,形成了4～5级中强地震反复发生的潜在震源区：在该断裂带主干上所发生的地震活动基本上具有前-主-余-震型和震群型的特点：在该断裂带主干上的M≥3．0以上的中等地震主要发生在北西向永安-晋江断裂的以南地区;该断裂带的地震活动在空间分布上是中段地震活动性强,北段地震活动性弱。 相似文献
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鲜水河断裂带多断层相互作用的流变断裂力学分析 总被引：3，自引：0，他引：3
本文研究了流变介质内多断层的相互影响,通过对鲜水河断裂带的分析,对该断裂带提出一个不共线三断层的断裂力学模型.把介质考虑成流变的,用有限元法结合解析方法求解了流变断裂力学问题的应力、应变及能量场的时空变化.结果表明,多断层的力学场与单一断层的力学场相差甚远,在断层间形成了影响区.在影响区内应力集中,梯度大,分布复杂,应变能在影响区内形成较大范围集中.应变能等值线在孕震期间从影响区向外扩张,能量从外围流向断层区,流动在时空上都是不均匀的,孕育初期增加速率大,后期渐渐平缓.流向影响区的能量比其周围区域大,形成很大梯度.并讨论了地震前兆的某些特征.根据本文的结果,认为在道孚-乾宁-带发生地震的可能性较大. 相似文献
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Boming Zhao Xiwei Xu School of Civil Engineering Beijing Jiaotong University Beijing China National Center for Active Fault Studies 《地震学报(英文版)》2009,(2):175-179
Major cases of the MS8.0 Wenchuan earthquake are obtained through field investigations of the epicenter and high-intensity areas, and the relationships among earthquake faults, ground motion and earthquake disasters near fault zones are analyzed.Both strong deformation and ground rupture lead to significant damages of the buildings, indicating that it is necessary to keep safe distance away from active faults and to take other necessary measures.There are two reasons for that the buildings near the surface ... 相似文献
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断裂活动和地震活动具有互为因果的关系,而不同于一般做法,文中用地震的活动性来分析断裂带的活动特征.为了解邯郸市周边存在的断裂带的活动特征,基于邯郸市附近地震台网监测的地震数据,利用地震纵波速度和震源位置联合反演方法,得到了邯郸市周边主要断裂带上地震波速度及震中在空间和时间上的分布特征,确定了地下壳质的纵波速度结构特征.综合分析表明:邯郸市周边小震的活动主要由磁县断裂和林州-武安断裂引起,太行山山前断裂带南端(邯郸-磁县段)几乎没有活动;地震活动集中在6 ～ 10km的范围内;活动时间特征是,从开始的2条断裂带同时活动逐渐演变为以磁县断裂活动为主. 相似文献
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Similarities between strike-slip faults at different scales and a simple age determining method for active faults 总被引：1，自引：0，他引：1
Abstract Several differently scaled strike‐slip faults were examined. The faults shared many geometric features, such as secondary fractures and linkage structures (damage zones). Differences in fault style were not related to specific scale ranges. However, it was recognized that differences in style may occur in different tectonic settings (e.g. dilational/contractional relays or wall/linkage/tip zones), different locations along the master fault or different fault evolution stages. Fractal dimensions were compared for two faults (Gozo and San Andreas), which supports the idea of self‐similarity. Fractal dimensions for traces of faults and fractures of damage zones were higher (D ～1.35) than for the main fault traces (D ～1.005) because of increased complexity due to secondary faults and fractures. Based on the statistical analysis of another fault evolution study, single event movements in earthquake faults typically have a maximum earthquake slip : rupture length ratio of approximately 10?4, although this has only been established for large earthquake faults because of limited data. Most geological faults have a much higher maximum cumulative displacement : fault length ratio; that is, approximately 10?2 to 10?1 (e.g. Gozo, ～10?2; San Andreas, ～10?1). The final cumulative displacement on a fault is produced by accumulation of slip along ruptures. Hence, using the available information from earthquake faults, such as earthquake slip, recurrence interval, maximum cumulative displacement and fault length, the approximate age of active faults can be estimated. The lower limit of estimated active fault age is expressed with maximum cumulative displacement, earthquake slip and recurrence interval as T ? (dmax /u) · I(M). 相似文献
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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 
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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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Resistivity mapping using the VLF-MT method around surface fault ruptures of the 1995 Hyogo-ken Nanbu earthquake, Japan 总被引：1，自引：0，他引：1
Abstract Distinctive fault ruptures, the Nojima Fault and Ogura Fault, appeared along the northwestern coast of Awaji Island at the time of the 1995 Hyogo-ken Nanbu earthquake (Kobe earthquake). In order to delineate the shallow resistivity structures around the faults just after they formed, Very Low Frequency Magnetotelluric (VLF-MT) surveys were made at five sites along the Nojima Fault and at one site along the Ogura Fault. Fourteen transects were made at the one site on the Ogura Fault, and another transect covers the area between the two faults. Changes in apparent resistivity or phase, or both, commonly occur when crossing the surface location of one of the faults, except for the northern transects at OGR-0 on the Ogura Fault. Apparent resistivity values of less than 100 Ωm were observed for Tertiary and Quaternary sediments and values larger than 200 Ωm for granitic rocks. The resistivity structures are related to the morphological characteristics of the fault ruptures. Remarkably conductive zones (less than 10 Ωm in apparent resistivity and 30–40 m in width) were found where the surface displacement is distinct and prominent along a single fault plane. If remarkably conductive zones were formed at the time of the 1995 Hyogo-ken Nanbu earthquake, the results provide a good constraint on the dimensions of a conductive zone near the surface that was made by one earthquake. Alternatively, if characteristic resistivity structures existed prior to the earthquake, the conductive zone was probably formed by some tens of earthquakes in relatively modern times. In this case, this phenomenon is inferred to be a concentration of fracturing in a narrow zone and is associated with the formation of clay minerals, which enhance rock conductivity. 相似文献
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Abstract Bathymetric data from south of Hokkaido obtained during a cruise of R/V Hakuho-Maru are summarized, and their correlation with earthquake occurrence is discussed. There are structural lineations on the seaward slope of the Kuril Trench, oblique to the Kuril Trench axis and parallel to the magnetic lineations in the Pacific plate. The structural lineations comprise horst-grabens generated by normal faulting. This suggests that Cretaceous tectonic structures originating at the spreading centre affect present seismotectonics around the trench axis. The structural-magnetic relation is compared to the case of the Japan Trench. North-east of the surveyed area, there are two major fracture zones (Nosappu Fracture Zone and Iturup Fracture Zone) that divide the oceanic plate into three segments. If the fracture zones (FZ) and the zone of paleo-mechanical weakness, represented by magnetic lineations, can control the direction of normal faults at a trench, the extent of the resulting topographic roughness on the seaward slope of the trench would be different across an FZ because of the differences in ages. By studying recent large earthquakes occurring in the south Kuril region, it is shown that several main-aftershock distributions for large earthquakes in this region are bounded by the Nosappu FZ and the Iturup FZ. Two models (Barrier model and Rebound model) are presented to interpret earthquake occurrence near the south Kuril Islands. The Barrier model explains seismic boundaries seen in several examples for earthquake occurrence in the south Kuril regions. The fracture zone forming the boundary of two segments with different magnetic lineations is also the boundary of two different normal fault systems on their ocean bottom, and the difference in sea-bottom roughness between two normal fault systems should affect the seismic coupling at a plate interface. Due to the difference of seismic coupling, earthquake occurrence is controlled by an FZ and then the FZ acts as a seismic boundary (Barrier model). Existing normal faults created by plate bending of subducting oceanic plate should rebound after its subduction (Rebound model). This rebound of normal faults may cause intraplate earthquakes with a high-angle reverse-fault mechanism such as the 1994 Shikotan Earthquake. The energy released by an intraplate earthquake generated by normal-fault rebounding is not directly related to that of interplate earthquakes such as low-angle thrust earthquakes. It is a reason why large earthquakes occurred in the same region during a relatively short period. 相似文献
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兰州地区活动构造的基本特征 总被引：5，自引：0，他引：5
兰州地区发育了NWW向和NWW向2组主导性活动构造带。大致以河口为界，东部地区主要为NWW向的马衔山－兴隆山左旋逆走滑活动断裂系，其新活动明显，是区内的主要控震断裂，1125年兰州7级地震就发生在其中的马衔山北缘断裂带的西端。河口以西为拉脊山北缘断裂和庄浪河断裂等1组NWW向的弧形逆冲断褶带，变形方式以断裂扩展褶皱为主，其新活动可能导致了138年金城－陇西63／4级地震、1440年永登61／4级地震和1995年永登5.8级地震的发生。兰州市区所在的兰州盆地则夹持在上述2组活动构造之间，其内同样发育了NWW向和NWW向的次级断裂，如刘家堡断裂、金城关断裂、雷坛河断裂及深沟桥断裂等，其上具有孕育和发生中强震的构造条件。 相似文献