共查询到20条相似文献，搜索用时 968 毫秒
1.
强震孕育和发生与较大空间尺度和时空演变的地壳运动,尤其是活动块体及其边界带的构造变形密切相关.Matsu'ura负位错模型认为受现今地壳运动驱动下的各活动地块间的相对运动在地块边界处有可能受到部分阻碍,从而导致应力应变积聚.若视块体边界区域的地表位移为刚性块体的(平移)运动减去边界上部(由若干断层段构成,每一断层段用弹性半空间的单一矩形位错模型模拟)对块体相对运动的部分锁定在地表产生的位移.则利用地表位移观测可将区域深部的多个块体与其边界断层联系起来,其通过反演确定的块体边界断层带的相对闭锁区,对地震预报很有意义.而实际存在的地壳变形还应包含块体本身的变形.本文研究建立一种块体弹性变形及其边界负位错部分锁定的水平形变复合作用模型,即增加块体应变参量.经比较研究,此模型较原Matsu'ura负位错模型及笔者以往所作的对模型的初步改进(增加块体旋转参量)更符合地壳运动实际,拟合效果大为改善;进而求取该复合模型形变应变场的时空演化图像,并借助年均应力降(主要反映剪应力强度)与年均地震矩(反映块体边界断层段的能量积累速率)度量断层锁定能量强度,其图像表现力和时空演变定量化程度大幅提高. 相似文献
2.
通过建立非震形变的位错模型,用混合全局反演方法,拟合了中国台湾南部1990-1995年间的GPS观测资料.根据地质构造和地震观测,构筑了包括6个刚性块体和19个断层的简单模型.反演结果表明,菲律宾海板块以(69±2)mm/a,方向为317°±2°的速度与欧亚板块会聚,其中约一半的会聚率在台东纵谷消耗掉,另外部分则平均分配在其西边的块体交界处.菲律宾海板块和中央山脉地质区均向西北方向挤压,过了中央山脉后,块体运动呈扇形分布,与应力方向一致.西部麓山地质区与滨海平原地质区交界处的断层均以逆冲分量为主,由南向北倾角逐渐变小,断层宽度一般为10km左右,均表现为强锁定,历史上的大地震多发生在这个地区. 相似文献
3.
通过对GPS观测资料的数值模拟，获取1999～2001年青藏块体东北缘地区地壳水平运动的非震反位错模型,结合本区视应变场空间分布，研究活动块体及其边界断裂运动、变形特征及应力应变积累部位和强度．结果表明:① 9个活动块体呈现东向由偏北至偏南的整体性顺时针运动. 以祁连山——海原断裂为界，两侧块体间的左旋相对运动明显，由西向东呈现走滑兼NE-NEE向挤压；② 有20条断层段（多数呈压性）不同程度地阻碍块体间的相对运动，其中祁连山断裂中东段（包括与日月山——拉脊山断裂交汇区）及与海原、庄浪河断裂交汇区更有利于应变积累，日月山——拉脊山断裂与柴达木块体北边界交汇区也可能存在一定程度的应变积累；③ 所得活动块体运动速率及边界断裂对块体相对运动的锁定量较1993～1999年相应结果有所减弱． 相似文献
4.
5.
以青藏高原北缘及东北缘的柴达木-祁连山地块内的活动断裂、由断裂所围限的微小块体为研究对象,系统收集整理区内活动断裂定量参数和GPS速度场等资料,使用球面应变率计算方法分析研究区内GPS 速度场得到现今构造应变率场,讨论区内最大剪应变率、面膨胀率与旋转率等参数与区域构造变形之间的关系;同时,依据区内详实的活动断裂资料建立精细的微小活动块体模型,利用Backslip模型反演断裂所围限的各个块体边界断裂的滑动速率、块体内部统一应变率及块体欧拉运动学参数等,并与活动构造方法获得的滑动速率做对比;最后,讨论研究区内由GPS速度场所揭示的地壳运动变形模式.结果表明:(1)柴达木-祁连山地区地壳运动,在沿着山脉走向上具有带状区域分块运动特征,大范围内具有弥散变形特征;(2)青藏高原北部变形场应是通过不同断裂差异性相对运动、区域内部逆冲挤压和块体旋转共同作用的结果.从鄂拉山到古浪民勤一带具有强烈的逆冲活动,其两侧地壳块体分别具有逆向旋转的运动性质;(3)在研究区东部GPS速度场所呈现顺时针旋转的形态,应是处于不同地块边界处的中下地壳与地幔介质差异驱动机制对上地壳块体所产生的作用,并以近地表断层应变率积累形式表现的结果,是祁连山地块、阿拉善块体、鄂尔多斯地块等大型块体推挤旋转影响下的复杂运动学形态. 相似文献
6.
《地震研究》2017,(3)
利用日本九州岛地区连续GPS观测数据,分析了2016年熊本M_W7.1地震前的区域地壳变形演化特征。GPS速度场和应变率场显示,熊本地震前右旋剪切应变积累区主要集中在断层上盘的九州中部块体(CKY)内,断层下盘的南海弧前块体(NFY)和九州南部块体(SKY)表现为显著的绕块体中心的逆时针刚性旋转运动;熊本地震发生在右旋剪切应变率高值区的边缘,且发震断层附近区域GPS应变时序结果显示自2014年后右旋剪切应变呈逐渐增强趋势;平行断层方向的GPS速度剖面结果显示发震断层上盘右旋剪切应变积累特征显著,表现为越靠近断层处的滑动速率越小,且断层西北侧站点速率随离开断层距离的增加呈非线性趋势变化。另外,GPS剖面结果显示,日奈久断层近场存在1~2 mm/a的相对滑动,可能存在浅层蠕滑运动。 相似文献
7.
现今中国大陆地壳运动与活动块体模型 总被引：68，自引：2，他引：68
通过分析中国地壳运动观测网络GPS数据特别是1999年与2001年区域网数据, 我们初步得到了中国大陆地壳运动速度场, 并用统计分析的方法从高密度台站速度场中区分出9个独立活动块体和2个广泛形变带, 求出活动块体刚体运动欧拉极和相邻块体间相互运动速率. 结果显示中国大陆形变场似可分为3类区域 第1类区包括青藏高原内部区域和天山造山带, 形变在全区域内广泛分布; 第3类区包括塔里木盆地及南北带以东地区, 形变场表现为活动块体, 内部稳定, 形变局限在狭窄的边界带内; 第2类区则处在青藏高原的边缘带, 如柴达木、祁连、西宁、川滇菱形南块体等, 这类区形变场特征处在第1, 3类区之间, 虽然还能保持一定的块体完整性, 但块体的尺度和强度已不如第3类地区. 通过分析各类区域岩石圈结构以及形变模式我们可以得出初步推断 中国大陆地壳形变模式主要由地壳结构所控制. 中国大陆东部和塔里木盆地地区地壳介质有相当强度, 形变表现为刚性块体的相互运动. 而印度板块的北向挤压造成青藏高原和天山的隆起并产生巨厚地壳, 壳内温度上升, 下地壳低速高导层发育, 介质呈较强黏塑性, 地壳脆性层在下地壳塑性流变场作用下产生各种类型的、多层次的形变, 且分布广泛而不局限于少量块体边界地区. 青藏高原边缘的第2类地区地壳结构为第1, 3类地区之间的过渡区, 其形变特征也介于第1, 3类地区之间, 为强度较低的较小活动块体在边界作用力下的运动与变形. 相似文献
8.
利用华北地区2009—2014年GPS水平运动速度场数据,采用块体负位错模型反演了郯庐断裂带中南段断层深部滑动速率、断层闭锁程度分布、断层滑动亏损速率分布及地震矩积累率,结合地表应变率分布,对郯庐断裂带中南段深、浅部形变、应变特征以及华北地区的地壳形变模式进行了分析.结果表明:郯庐断裂中南段的北端主要为右旋走滑特性,南端则表现为右旋走滑兼拉张性运动,断层滑动速率在0.9mm·a~(-1)至1.2mm·a~(-1),且沿断层走向由北至南逐次增大.断层闭锁程度分布沿走向分布不均一,断层闭锁深度由最北端的27km增加到中段的32km,至最南端变为5km,断层闭锁最深处与1668年郯城MS8.5震中位置相对应.断层滑动亏损速率沿走向由0.9mm·a~(-1)增加到1.2mm·a~(-1),沿倾向由地表至深部逐渐减小为0mm·a~(-1).地震矩积累率在郯庐断裂带中南段郯城附近较大,而地表对应区域为第二应不变分量的低值区.华北地区地壳变形以块体运动为主,块体内部应变及断层闭锁产生的负位错效应次之;郯庐断裂带中南段断层形变沿走向呈条带状分布,形变宽度单侧小于50km,形变量不超过1mm·a~(-1),且上盘形变略大于下盘. 相似文献
9.
目前很多文献基于弹性力学假设,以小形变、均匀应变场为前提,利用GPS资料建立了中国大陆块体的整体旋转与均匀应变模型,并对模型进行了相关检验.但上述对模型的检验侧重从模型的拟合效果上进行分析和比较,忽略了对模型的适用性和假设条件合理性的检验.实际上,不同块体由于自身构造和外部条件的不同,其运动状况与应变状态并不完全一致,模型的适用性需进一步的验证.本文提出了两步检验方法对所建立的模型在中国大陆6个主要块体上进行了检验：第一步对应变参数进行显著性检验,第二步对应变均匀性进行检验,结果表明：根据所用数据精度,华南块体的刚性程度在95% 的置信水平上可以认为显著的,建立模型时不必考虑内部形变;其他块体内部形变显著,整体旋转与均匀应变模型并不能反映真实的地壳运动状态,必须考虑其形变的不均匀性. 相似文献
10.
利用青藏块体东北缘地区1999～2001年GPS观测获得的地壳水平运动速率场,通过对该地区进行块体划分,将该地区划分为9个块体,应用块体的整体旋转线性应变模型(RELSM)估计了各个块体的旋转与应变参数,以及计算了该地区内143个GPS站点的应变参数,以此分析了该地区的应变场的基本特征,结果表明:①阿拉善块体s较稳定,其旋转角为0.630×10-8,运动速率为0.688 mm/a,②相比其他块体,共和块体旋转角最大达到了6.589×10-8 ,运动速率达到了7.296 mm/a,③应变高值区主要集中在祁连山断裂,海原断裂等,在这些地区最大剪应变率达到了7.5×10-8、面膨胀率达到了-2.5×10-8、主压应变达到了-6×10-8. 相似文献
11.
The GPS data in and around the Ordos block area indicate that the left-lateral slip rate along the northern or southern margin of the Ordos block is about twice or three times as fast as the right-lateral slip rate along the eastern or western margin of the block. However, many researchers stressed the dextral-slip of the eastern or western boundaries of the Ordos block, and suggested that the block as a whole rotated counterclockwise based on the available geological data. Focusing on the inconsistency, we reexamine the late Cenozoic deformation pattern in the Ordos region based on seismicity data and geodesy data (GPS and leveling) around it. The results indicate that the rigid block-like motion appears to be the basic characteristic of the kinematics of the Ordos region, and this motion is absorbed by the displacement of the faults around the block. When the faults along the northern and southern boundaries of the Ordos block are active, its eastern boundary is inactive. However, if the faults along the eastern boundary are active, the northern and southern are inactive. In recent years, the northern and southern boundaries of the Ordos block are in active. But in the long term, the Ordos block is moving southeastward relative to the Alxa and Yinshan blocks because of the strong pushing of the Tibetan Plateau on its southwestern side, and this deformation is accommodated by the counterclockwise rotation of the block itself. 相似文献
12.
The GPS data in and around the Ordos block area indicate that the left-lateral slip rate along the northern or southern margin of the Ordos block is about twice or three times as fast as the right-lateral slip rate along the eastern or western margin of the block. However, many researchers stressed the dextral-slip of the eastern or western boundaries of the Ordos block, and suggested that the block as a whole rotated counterclockwise based on the available geological data. Focusing on the inconsistency, we reexamine the late Cenozoic deformation pattern in the Ordos region based on seismicity data and geodesy data (GPS and leveling) around it. The results indicate that the rigid block-like motion appears to be the basic characteristic of the kinematics of the Ordos region, and this motion is absorbed by the displacement of the faults around the block. When the faults along the northern and southern boundaries of the Ordos block are active, its eastern boundary is inactive. However, if the faults along the eastern boundary are active, the northern and southern are inactive. In recent years, the northern and southern boundaries of the Ordos block are in active. But in the long term, the Ordos block is moving southeastward relative to the Alxa and Yinshan blocks because of the strong pushing of the Tibetan Plateau on its southwestern side, and this deformation is accommodated by the counterclockwise rotation of the block itself. 相似文献
13.
台湾是菲律宾海板块与欧亚板块会聚、碰撞的产物,区内地质构造复杂,地震频发,变形强烈.为定量研究台湾地区变形特征及其动力学成因,文中运用二维不连续变形体弹性力学的有限单元计算方法,利用台湾地区1995—2005年GPS的观测结果作为边界约束,对台湾地区地壳变形场进行了模拟.计算结果显示,台湾中部地区主要呈压缩状态,但在台湾的东北部及南部地区出现了拉张的变形环境.变形程度最大的区域位于台湾东部海岸山脉及其附近海域,同时,计算给出台湾纵谷断裂滑移速率约为13.8~23.5mm/yr,由于纵谷断裂对变形的吸收,因此变形在纵谷断裂以西及西北地区迅速衰减.此外,计算结果还发现,计算给出的台湾岛上的速度值与GPS观测结果吻合得较好;计算给出的主应力方位与地应力观测及震源机制解结果也颇为一致.由此说明文中的有限元模型是合理的.此外,计算结果还表明,菲律宾海板块向北西方向的推挤,板块边界形状,观音、北康高地的抵阻,冲绳海槽扩张及琉球海沟的向南后撤以及断裂作用等,共同造成了台湾地区现今变形场的主要格局. 相似文献
14.
Ｒｅｇｉｏｎａｌｃｈａｒａｃｔｅｒｉｓｔｉｃｓｏｆｓｔｒｅｓｓｆｉｅｌｄｉｎｔｈｅｓｏｕｔｈｅｒｎｐａｒｔｏｆｔｈｅｎｏｒｔｈ－ｓｏｕｔｈｓｅｉｓｍｉｃｂｅｌｔｉｎＣｈｉｎａａｎｄｉｔｓｒｅｌａｔｉｏｎｗｉｔｈｐｌａｔｅ ｍｏｖｅｍｅｎｔＪｉ－Ｒｅｎ... 相似文献
15.
Introduction So small is the hypocenter area of strong earthquake, but its formation is controlled by time-space evolution of present-day crustal movement in wider-range area, and related to motion and deformation of active blocks and their boundary faults. Aseismic negative dislocation model presented by Matsuura, et al (1986) is that, the relative motion between blocks driven by present-day crustal movement may be partly locked at the block … 相似文献
16.
使用2011年8月至2012年8月在南北地震带南段布设的密集流动地震台站记录的波形数据,采用绝对定位方法对滇西地区的1593个地震进行了初步定位,应用近震走时层析成像方法获得了滇西地区三维地壳P波速度结构。研究结果表明,攀枝花附近的高速异常从地表可一直延伸至中地壳,并在中下地壳深度与滇西北地区的高速异常形成大范围的高速块体。这一高速异常体对青藏高原物质向南逃逸起到一定的阻挡作用,可能是导致川滇活动块体北部次级块体快速抬升的重要因素。位于印度板块与欧亚板块俯冲边界的腾冲、保山地块在下地壳表现为明显的大范围低速异常,推测该低速异常与印度板块东向俯冲引起的地幔热物质上涌有关。金沙江-红河断裂带是川滇块体重要的南部边界,红河断裂带中段的弥渡至红河一带具有高速的地壳结构以及较弱的地震活动性,可能表明该区现阶段处于闭锁状态,是未来需要重点监测的地段之一。 相似文献
17.
18.
于慎谔 《地震学报(英文版)》2004,17(4):417-425
Introduction Shanxi fault depression zone (SFDZ) is one of important Cenozoic fault basin zones and strong earthquake belts in Chinese mainland. Its northern part has aroused wide research interests due to the complicated tectonics and high activity of strong earthquakes there. Early researches on this depression zone were carried out since 60s of last century (DENG, et al, 1973; DENG, YOU, 1985; LU, DING, 1985; XU, 1990; XU, et al, 1996, 2002). In 90s of last century, the geologica… 相似文献
19.
20.
CHARACTERISTICS OF FOCAL MECHANISMS AND STRESS FIELD IN THE EASTERN BOUNDARY OF SICHUAN-YUNNAN BLOCK AND ITS ADJACENT AREA 
下载免费PDF全文
下载免费PDF全文 This study is devoted to a systematic analysis of the stress state of the eastern boundary area of Sichuan-Yunnan block based on focal mechanisms of 319 earthquakes with magnitudes between M3.0 and M6.9, occurring from January 2009 to May 2018. We firstly determined the mechanism solutions of 234 earthquakes by the CAP method, using the broadband waveforms recorded by Chinese regional permanent networks, and collected 85 centroid moment tensor solutions from the GCMT. Then we investigated the regional stress regime through a damp linear inversion. Our results show that:1)the focal mechanisms of moderate earthquakes are regionally specific with three principal types of focal mechanisms:the strike-slip faulting type, the thrust faulting type and the normal faulting type. The strike-slip faulting type is significant in the eastern boundary area of Sichuan-Yunnan block along the Xianshuihe-Xiaojiang Fault, the Daliangshan Fault, and the Zhaotong-Lianfeng Fault. The thrust faulting type and the combined thrust/strike-slip faulting type are significant along the Mabian-Yanjin Fault, Ebian-Yanfeng Fault and the eastern section of Lianfeng Fault; 2)The most robust feature of the regional stress regime is that, the azimuth of principal compressive stress axis rotates clockwise from NWW to NW along the eastern boundary of Sichuan-Yunnan Block, and the clockwise rotation angle is about 50 degrees. Meanwhile, the angels between the principal compressive axis and the trend of eastern boundary of Sichuan-Yunnan Block remain unchanged, which implies a stable coefficient of fault friction in the eastern boundary fault zone of Sichuan-Yunnan Block. The movement of the upper crust in the southeastern Tibetan plateau is a relatively rigid clockwise rotation. On the whole, the Xianshuihe-Xiaojiang Fault is a small arc on the earth, and its Euler pole axis is at(21°N, 88°E). The Daliangshan Fault is surrounded by the Anninghe-Zemuhe Fault, which formed a closed diamond shape. When the Sichuan-Yunnan block rotates clockwise, the Daliangshan Fault locates in the outer of the arc, while the Anninghe-Zemuhe Fault is in the inward of the arc, and from the mechanical point of view, left-lateral sliding movement is more likely to occur on the Daliangshan Fault. Our results can be the evidence for the study on the "cut-off" function of the Daliangshan Fault based on the stress field background; 3)The regional stress regime of the eastern boundary faults zone of the Sichuan-Yunnan Block is the same as the south section of the Dalianshan Fault, and the focal mechanism results also reveal that the Dalianshan Fault is keeping left-lateral strike-slip. There may be the same tectonic stress field that controls the earthquake activities in the southern section of Daliangshan Fault and Zhaotong-Lianfeng Fault. The regional stress regime of Zhaodong-Lianfeng Fault is also the same with the Sichuan-Yunnan Block, which implies that the control effect of the SE movement of the Sichuan-Yunnan block may extend to Weining. 相似文献