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1.
正郯庐断裂带山东段又称沂沭断裂带,发生了中国大陆东部最大历史地震,即1668年郯城级地震,安丘—莒县断裂是其主要的破裂段;该断裂现代小震密集成带,显示深部破裂区仍未愈合。野外考察显示,位于莒南县左山次级破裂段出露长度8 km,走向N15—20°E,倾向南东,倾角70°—80°,其中位于莒南县岭泉镇左山村西的地震断层遗址显示,山脊断错接近10 m。沂沭断裂带作为郯庐深大断裂的一部分,由4条主干断裂组成了"两堑夹一垒"构造形  相似文献   

2.
郯庐断裂带的分段与沂沭断裂的活动性   总被引:8,自引:0,他引:8  
郯庐断裂带是中国东部的主要强震构造带,活动性分段明显,大致可分:黑龙江鹤岗—铁岭段,为弱活动深震、中深震段;下辽河—莱州湾段,为强活动、高频强震段;鲁苏沂沭段,为强活动、低频强震带和南部大别山—广济的弱活动弱震段。其中鲁苏沂沭段中规模最大的沂沭断裂带,在第四纪以来的新构造活动分段尤为明显,以临沂汤头至莒南大店一线为界,北部以高角度正断或逆冲、蠕滑为主。在活动时代上早于或相当于更新世晚期。南部除更新世活动外,全新世以来至少有三次强活动迹象。而且从莒南岭泉的左山至新沂何庄,延续 120公里范围内有1668年郯城8.5级地震形变带和地震断层,这也是郯庐断裂带的最新活动段。  相似文献   

3.
郯庐断裂带穿越中国东部鲁、苏、皖等3省,文中称此段为郯庐断裂带鲁苏皖段。通过地震地质、深地震勘探、天然地震层析成像、地震活动、地貌和现今地壳运动速度场等方面资料的分析和对比研究,根据历史地震重演原则和地质构造类比原则,对郯庐断裂带鲁苏晥段未来强震的可能发生地段进行了探讨。泗洪南(王集)—嘉山一带与1668年郯城8级地震震中地区对比分析发现,两处在深、浅部地质构造、新构造运动、地震活动性等方面存在较大的相似性。结合郯庐断裂带鲁苏皖段7级及以上强震的分布及其重现周期等方面综合分析,初步认为,郯庐断裂带鲁苏皖段在泗洪南(王集)—嘉山一带存在发生7级或7级以上强地震的可能性。  相似文献   

4.
沂沭断裂带内部的差异活动及其成因分析   总被引:8,自引:0,他引:8  
郯庐断裂带在山东境内被称为沂沭断裂带的部分是其新构造活动最为强烈的一段.许多学者对沂沭断裂带做过大量研究工作,指出沂沭带活动存在差异性,但较少关于差异活动的原因分析.本文在前人研究工作基础上,较为深入地分析了沂沭带5条断裂的主要活动规律及其特点,对沂沭带进行了新的分段,并归纳了沂沭带不同断裂之间、同一断裂不同段落之间的活动差异及其差异的基本特征.在此基础上,从地貌、断裂结构、断裂空间组合、现代运动、深部构造环境等几个方面,分析阐述了造成沂沭带差异活动的可能原因,为更深入地研究沂沭带提供了新鲜的启示和思路.  相似文献   

5.
1 研究背景 郯城—庐江断裂带(郯庐断裂带)是我国东部规模最大、延伸最长的深大断裂带,也是我国地震危险性最高的断裂构造之一.据史料记载,1668年郯城8?级地震(史称郯城大地震,位于郯城、临沂、临沭三县交界处)发生在该断裂潍坊—嘉山段郯城附近.近年来,郯庐断裂带第四纪活动地质证据被陆续发现,如郯庐断裂带江苏段全新世活动(曹筠等, 2018)以及郯庐断裂带北段(依兰—伊通断裂黑龙江通河段、吉林舒兰段,以往认为不具活动性)第四纪晚期活动证据(闵伟等,2013).此外,一些原有第四纪活动段,如新沂—五河段、乌云山—合肥段(郑颖平等,2014)等,也在近年被发现了活动证据.  相似文献   

6.
郯庐断裂带莒县胡家孟晏地震破裂带的发现   总被引:4,自引:3,他引:1       下载免费PDF全文
郯庐断裂带是中国东部最主要的一条活动断裂带。在该断裂带中部,沂沭断裂东地堑的潍坊—嘉山段中发育了1条长360km的全新世活动断裂带(F5),在该全新世断裂带的北段和中段分别发生了公元70年的安丘地震和公元1668年的郯城地震。2003年底我们考察沭河断裂带时,在莒县境内发现了1条长约7km的地震破裂带,作为活动断层应该归属于F5断裂带,但其是一条独立的地震破裂段还是归属于1668年郯城8.5级地震破裂带有待于进一步的研究。尽管如此,探槽揭示出的上覆未经破坏的地层的14C年代表明,该破裂带在(2140±190)aBP以来没有过活动,因此我们认为其作为1条独立破裂段的可能性较大  相似文献   

7.
郯庐断裂带地震活动特征   总被引:2,自引:0,他引:2  
本文较为详细地研究了郯庐断裂带及附近地区的地震活动,其主要结果为:1、郯庐断裂带地震活动由四个地震活动区段组成,该带活动的主体区段是那城─—渤海─—海城.2、郯庐断裂带地震活动的周期性是形成邦城─—海城区段中强地震活动的主要原因.3、郯庐断裂带中北段(邦城─—海城)M≥6.0级地震具有较好的迁移规律.4、郯庐断裂带近代小震活动表现出南段随机性,中段呈线性,北段具有密集区带性等特点。5、郯庐断裂带震源深度表现出南、北段浅,中段深,且散度大的特点。6、郯庐断裂带Q值分布表明,沂沭带介质强度的完整性较差。  相似文献   

8.
以往对郯庐断裂带沂沭段各条断层第四纪活动性研究工作都集中在有历史地震记录的东地堑断层,而对断裂带西地堑断层却极少涉及,仅有的关于西地堑2条断层活动性的研究也至今没有定论。针对沂沭断裂带南段西地堑2条断层开展系统的浅层地震勘探和钻孔联合剖面相结合的研究,明确了鄌郚-葛沟断裂(F4)可能是第四纪早期断裂,而活动性较强的沂水-汤头断裂(F3)属于晚更新世活动断裂,其最新1次活动时间发生在距今(91.2±4.4)~(97.0±4.8)ka。结合断裂带其他断层的最新研究成果,对比东、西地堑活动断层最新活动时间,揭示出沂沭断裂带南段晚第四纪活动是断裂带对来自两侧应力的构造响应。沂水-汤头断裂可能是该区域未来中强地震的潜在发震构造。  相似文献   

9.
郯庐断裂带是中国东部最大的一个活动构造带,其内部结构非常复杂,不同区段表现出不同特征的构造样式.本文采用浅层地震反射波成像技术对郯庐断裂带宿迁段的近地表结构进行了高分辨率成像,利用该区已有的深地震反射剖面数据,采用初至波层析成像方法获得了郯庐断裂带的浅层P波速度结构.结果表明,郯庐断裂带宿迁段是一个由多条断裂以及凹陷和隆起构成的复杂构造带,且新生代地层厚度和地震波速分布明显受到断裂的影响与控制.郯庐断裂带的东、西两侧为基底隆起区,近地表速度结构呈现为明显的高速特征,新生代地层厚度小于200m.郯庐断裂带总体显示为低速凹陷结构,新生代地层厚度在300~600m之间变化,最厚处位于宿迁市的陵城镇附近.郯庐断裂带宿迁段主要由5条断裂构成,从这些断裂的上断点埋深和第四纪活动特征来看,郯庐断裂带的东边界断裂F_1和西边界断裂F_4的活动性相对较弱,为第四纪早期活动断裂.断裂F_2和F_3控制了郯庐断裂带内部的新生代凹陷,两者的活动时代分别为中更新世和晚更新世.安丘—莒县断裂F_5位于断裂F_1和F_2之间,由2条相向而倾的分支断层F_5和F_(5-1)构成,其活动时代分别为全新世和晚更新世.研究结果为进一步认识郯庐断裂带宿迁段的近地表特征及其活动性提供了新证据.  相似文献   

10.
郯庐断裂带鲁苏皖段主要是沂沭断裂带,该段自东向西分布着5条断裂.该段及邻区在大地构造位置上跨越中朝断块、扬子断块和秦岭-大别褶皱带3个一级构造单元,是多个构造单元的交汇部位.  相似文献   

11.
用多震相地震走时成像法反演郯庐断裂带鲁苏皖段及邻区三维地壳速度结构。一些地区如郯庐断裂带临沭到定远及以东地区在中地壳的20~25km出现低速层,一些地区莫霍面埋深有变化。浅层速度结构的分段与断裂活动的分段相一致,表明新沂到泗洪是活动断裂的闭锁段。对比1668年山东郯城8级地震区和研究区的深部速度结构,结合与郯庐带相交的断裂、地震活动、活动断裂的闭锁段、中地壳低速层及莫霍面深度变化,综合判断郯庐断裂带江苏段未来可能发生大震的地区为33.4°~34.1°N,118.2°~118.8°E,重点是宿迁、沭阳、泗阳和泗洪。震级估计可达8级。  相似文献   

12.
安丘-莒县断裂是沂沭断裂带最主要的活动断裂,对强震的发生具有明显的控制作用。该断裂的安丘—朱里段由南流段、双官—眉村段和朱里段3条右阶斜列的次级断裂所组成,以右旋走滑活动为主,兼有正断或逆冲活动分量;其最新活动时代推断为晚更新世—全新世早期。根据断裂活动性的最新研究成果,认为在莒县至昌邑之间安丘-莒县断裂仍是占主导地位的活动断裂,与公元前70年安丘7级地震的发生具有密切关系  相似文献   

13.
The May 12, 2008 MS7.9 Wenchuan earthquake is ranked as one of the most devastating natural disasters ever occurred in modern Chinese history. The Longmenshan Fault(LMSF) zone is the seismogenic source structure, which consists of three sub-parallel faults, i.e., the Guanxian-Jiangyou Fault(GJF) in the frontal, the Yingxiu-Beichuan Fault(YBF) in the central fault and the Wenchuan-Maowen Fault(WMF) in the back of the LMSF. In this study, geological survey and seismic profiles are used to constrain the faults geometry and medium parameters. Three visco-elastic finite element models of the LMSF with different main faults are established. From the phase of interseismic stress accumulation to coseismic stress release and postseismic adjustment, the Wenchuan earthquake is simulated using Continuous-Discrete Element Method(CDEM). Modeling results show that before the 2008 Wenchuan earthquake, the GJF becomes unstable due to the interaction between its unique fault geometry and the tectonic stress loading. In the fault geometry model, the GJF is the most gently dipped fault among the three faults, which in return makes it having the smallest normal stress and the greatest shear stress. The continuous shear stress loading finally meets the fault failure criteria and the Wenchuan earthquake starts to initiate on the GJF at the depth of 15~20km. The earthquake rupture then propagated to the YBF. At the same time, due to the GJF and YBF rupture, the interseismic stress accumulation has been greatly reduced, causing the WMF failed to rupture. Although the stress accumulation in the WMF has been reduced significantly after the earthquake, yet it has not been released completely, which means that the WMF likely has with high seismic risk after the 2008 Wenchuan earthquake. We also find that the stress perturbation caused by gently dipping segment of the fault can promote the passive rupture in the steeply dipping segment, making the upper limit of dip angles larger than traditional assumption.  相似文献   

14.
On May 12, 2008, a magnitude 7.9 earthquake ruptured the Longmenshan fault system in Sichuan Province, China, collapsing buildings and killing tens of thousands people. As predicted, aftershocks may last for at least one year, and moreover, large aftershocks are likely to occur. Therefore, it is critical to outline the areas with potential aftershocks before reconstruction and re-settling people as to avoid future disasters. It is demonstrated that the redistribution of stress induced by an earthquake should trigger successive seismic activity. Based on static stress triggering theory, we calculated the coseismic stress changes on major faults induced by the Wenchuan earthquake, with elastic dislocation theory and the multilayered crustal model. We also discuss the stress distribution and its significance for future seismic activity under the impact of the Wenchuan earthquake. It is shown that coulomb failure stress (CFS) increases obviously on the Daofu-Kangding segment of the Xianshuihe Fault, the Maqu and Nanping segment of the Eastern Kunlun Fault, the Qingchuan Fault, southern segment of the Minjiang Fault, Pengxian-Guanxian Fault, Jiangyou-Guangyuan Fault, and Jiangyou-Guanxian Fault. The increased stress raises the probability of earthquake occurrence on these faults. Since these areas are highly populated, earthquake monitoring and early disaster alarm system are needed. CFS increases with a magnitude of 0.03–0.06 MPa on the Qingchuan Fault, which is close to the northern end of the rapture of Wenchuan earthquake. The occurrence of some strong aftershocks, including three events with magnitude higher than 5.0, indicates that the seismic activities have been triggered by the main shock. Aftershocks seem to migrate northwards. Since the CFS change on the Lueyang-Mianxian Fault located on the NEE of the Qingchuan Fault is rather small (±0.01 MPa), the migration of aftershocks might be terminated in the area near Hanzhong City. The CFS change on the western Qinling Fault is around 10 Pa, and the impact of static triggering can be neglected. The increment of CFS on the Pengxian-Guanxian Fault and Beichuan-Yingxiu Fault southwest to the main rupture is 0.005–0.015 MPa, which would facilitate earthquake triggering in these areas. Very few aftershocks in these areas indicate that the accumulated stress has not been released sufficiently. High seismic risk is predicated in these areas due to co-seismic CFS loading. The Wenchuan earthquake released the accumulated CFS on the Fubianhe Fault, the Huya Fault, the Ha’nan-Qingshanwan Fault, and the Diebu-Bailongjiang Fault. The decrement of CFS changes on the Longquanshan Fault east to Chengdu City is about 0.002 MPa. The seismic activity will be depressed by decrement of CFS on these faults. Supported by Knowledge Innovation Program of Chinese Academy of Sciences (Grant No. KZCX-SW-153), National Natural Science Foundation of China (Grant Nos. 40574011 and 40474028)  相似文献   

15.
In this paper, based on a large number of cumulative observational data from the seismic monitoring network in China, we grid the research area to calculate the density values at each grid node and convert the qualitative earthquake epicenter distribution to quantitative seismic pattern. Minimum magnitude of completeness(MC)is determined by magnitude-rank analysis, which provides lower limit earthquake and original time. New satellite-derived gravity model v23.1, which is based on satellites CryoSat-2 and Jason-1 data, is used to determine the Bouguer gravity anomaly derived from free-air gravity anomaly and elevation database sets SRTM30, and ultimately, the complete Bouguer correction is obtained. In this paper, the Xingtai earthquake zone and Tanlu fault zone (Anhui segment) are selected for case study. Bouguer gravity anomaly presents a NE-trending U-shaped narrow strip in the Xingtai earthquake zone, and its location is consistent with Shulu Fault Basin. Grid density value contours are restricted by the U-shaped strip, and the extreme value of seismic activity density lies in the bottom of the U-shaped strip as shown in the cross section. The results of Bouguer gravity anomaly and upward continuations to the different heights show good linearity and gradient in the Tanlu fault zone (Anhui segment); and both long-axis direction of seismic pattern and nodal plane strike of seismogenic fault from focal mechanism solutions trend NNE. In short, the Tanlu fault zone(Anhui segment)is a large deep-seated fault that still has the ability to control seismic activity along it. Based on the measured gravity and magmatic data, using the edge detection TDX method to interpret the concealed boundary of the Anqing M4.8 earthquake near the Tanlu fault, and combining with the results from deep seismic reflection profiles of the study area, we discussed the causative fault of the Anqing earthquake.  相似文献   

16.
快速确定断层破裂特征是烈度速报的一项重要技术,断层破裂特征可为烈度速报提供震源模型,提升烈度速报准确性。通过汶川地震加速度记录,提出一种快速计算震源破裂参数的方法。 假定断层为线源模型,以一定间距将断层离散化为若干子源,以震中为不动点,通过旋转获得所有断层可能的走向,通过每次移动一个子源,获得断层所有可能的破裂方式,将二者结合即可给出断层所有可能的空间分布;计算每种断层空间分布与每个台站的断层距,利用加速度记录峰值和断层距统计回归衰减关系,分析每个衰减关系的拟合残差,残差最小拟合效果最好的衰减关系所对应断层参数,能够对该次地震的地震动场有最合理的解释,也最有可能是实际地震中的断层空间分布。  相似文献   

17.
在汶川MS8.0级大震发生前一周,采用水压致裂技术在龙门山发震断裂带±400 m深度上测得的最大水平主应力值为21~22 MPa,与其附近下盘之差高达8~10 MPa.大震后的原地重复测量结果表明,发震断裂带上的最大、最小水平主应力值分别降低了29%和23%,而在下盘大震前后的地应力作用状况并无变化.测量结果分析表明,活动断裂带的地应力高值异常是圈定地震危险区的可靠依据,是强震孕育和发生的警示标志.  相似文献   

18.
2013年4月20日发生在龙门山南段的芦山MS7.0地震是继发生在龙门山中北段的汶川MS8.0地震之后的又一次强震。本文通过震后地表变形特征、余震分布、震源机制解、石油地震勘探剖面、历史地震数据等资料,结合前人对龙门山南段主干断裂、褶皱构造特征的研究以及野外实地考察,应用活动褶皱及"褶皱地震"的相关理论,初步分析芦山地震的发震构造模式。认为芦山地震为典型的褶皱地震,发震断裂为前山或山前带一隐伏断裂。构造挤压产生的地壳缩短大部分被褶皱构造吸收。认为龙门山南段前缘地区具有活褶皱-逆断层的运动学特征,表明龙门山逆冲作用正向四川盆地内部扩展。  相似文献   

19.
This paper reports the internal structures of the Beichuan fault zone of Longmenshan fault system that caused the 2008 Wenchuan earthquake, at an outcrop in Hongkou, Sichuan province, China. Present work is a part of comprehensive project of Institute of Geology, China Earthquake Administration, trying to understand deformation processes in Longmenshan fault zones and eventually to reproduce Wenchuan earthquake by modeling based on measured mechanical and transport properties. Outcrop studies could be integrated with those performed on samples recovered from fault zone drilling, during the Wenchuan Earthquake Fault Scientific Drilling (WFSD) Project, to understand along-fault and depth variation of fault zone properties. The hanging wall side of the fault zone consists of weakly-foliated, clayey fault gouge of about 1 m in width and of several fault breccia zones of 30–40 m in total width. We could not find any pseudotachylite at this outcrop. Displacement during the Wenchuan earthquake is highly localized within the fault gouge layer along narrower slipping-zones of about 10 to 20 mm in width. This is an important constraint for analyzing thermal pressurization, an important dynamic weakening mechanism of faults. Overlapping patterns of striations on slickenside surface suggest that seismic slip at a given time occurred in even narrower zone of a few to several millimeters, so that localization of deformation must have occurred within a slipping zone during coseismic fault motion. Fault breccia zones are bounded by thin black gouge layers containing amorphous carbon. Fault gouge contains illite and chlorite minerals, but not smectite. Clayey fault gouge next to coseismic slipping zone also contains amorphous carbon and small amounts of graphite. The structural observations and mineralogical data obtained from outcrop exposures of the fault zone of the Wenchuan earthquake can be compared with those obtained from the WFSD-1 and WFSD-2 boreholes, which have been drilled very close to the Hongkou outcrop. The presence of carbon and graphite, observed next to the slipping-zone, may affect the mechanical properties of the fault and also provide useful information about coseismic chemical changes.  相似文献   

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