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1.
为深入理解汶川地震破裂的构造运动机制,本文选取典型的观测点,利用多种地质地貌标志测绘分析得到了汶川Ms8.0地震发震断裂的近地表三维同震滑移矢量.结果显示,北川-映秀断裂上的白水河-高川破裂段北西盘沿88°方位角水平滑移2.58 m、垂直滑移3.70 m;安县-灌县断裂上的白鹿-汉旺破裂北西盘沿134°方位角水平滑移1.63 m,垂直滑移2.00 m;小鱼洞破裂带南西盘沿76°~79°方位角水平滑移2.15~2.71 m,垂直滑移1.36~1.51 m.平行的白水河-高川破裂段和白鹿-汉旺破裂段合计形成1.72 m右旋走滑和3.49 m垂直断裂带的NW向水平缩短,总滑移方向(106°)与断裂带整体走向(42°)呈64°夹角,整个龙门山推覆构造带处于斜向挤压的构造环境.结合震源过程反演成果的分析显示,斜滑的白水河-高川破裂段和逆冲型白鹿-汉旺破裂段可能是在汶川地震中最大的一次子事件过程以滑移分解的形式而同时破裂形成的,滑移分解作用使两条断裂以斜滑与逆冲组合的力学性质产生破裂而非相同件质的斜滑破裂.小鱼洞破裂以低角度斜滑为主,可能是安县-灌县断裂与北川-映秀断裂以滑移分解形式同时破裂的纽带.小鱼洞断裂是龙门山断裂带长期处于斜向挤压的构造环境的产物,不只是逆冲断裂系中的捩断层.  相似文献   

2.
为深入理解汶川地震破裂的构造运动机制,本文选取典型的观测点,利用多种地质地貌标志测绘分析得到了汶川MS8.0地震发震断裂的近地表三维同震滑移矢量.结果显示,北川—映秀断裂上的白水河—高川破裂段北西盘沿88°方位角水平滑移2.58 m、垂直滑移3.70 m;安县—灌县断裂上的白鹿—汉旺破裂北西盘沿134°方位角水平滑移1.63 m,垂直滑移2.00 m;小鱼洞破裂带南西盘沿76°~79°方位角水平滑移2.15~2.71 m,垂直滑移1.36~1.51 m.平行的白水河—高川破裂段和白鹿—汉旺破裂段合计形成1.72 m右旋走滑和3.49 m垂直断裂带的NW向水平缩短,总滑移方向(106°)与断裂带整体走向(42°)呈64°夹角,整个龙门山推覆构造带处于斜向挤压的构造环境.结合震源过程反演成果的分析显示,斜滑的白水河—高川破裂段和逆冲型白鹿—汉旺破裂段可能是在汶川地震中最大的一次子事件过程以滑移分解的形式而同时破裂形成的,滑移分解作用使两条断裂以斜滑与逆冲组合的力学性质产生破裂而非相同性质的斜滑破裂.小鱼洞破裂以低角度斜滑为主,可能是安县—灌县断裂与北川—映秀断裂以滑移分解形式同时破裂的纽带.小鱼洞断裂是龙门山断裂带长期处于斜向挤压的构造环境的产物,不只是逆冲断裂系中的捩断层.  相似文献   

3.
汶川8级大地震的地表破裂特征及分段   总被引:6,自引:1,他引:5  
2008年5月12日14时28分,四川省汶川县境内发生MS8.0地震.地表破裂多以跌水、陡坎形态发育在河流沟谷或晚新生代沉积层内,位移明显.山地受崩塌、滑坡影响,位移量较难获得.发震断裂主要有三条,即北川-映秀断裂、彭县-灌县断裂和小鱼洞断裂.北川-映秀断裂地表破裂由南向北活动性质从逆冲为主逐渐转变为走滑为主,长约220 km,平均垂直位移量约3 m,按位移量沿断裂走向的变化可以分为虹口段、北川段和南坝段;彭县-灌县断裂地表破裂以逆冲活动为主,长约82 km,平均垂直位移量约1.5 m,可以划分为白鹿段和汉旺段,断裂断距分布的几何特征与北川-映秀断裂的中南段相近;小鱼洞断裂是一条新生北西走向的次级破裂,长约5.6 km,平均垂直位移量约1.5 m,调节两侧构造单元变形差异,具有捩断层特征,活动以逆(左行)走滑为主,可划分出小鱼洞段和中坝段.姚都镇地表破裂可能说明南坝以北的地震具有不同的活动特征.活动断裂的运动方式反映区域应力场有北西西向挤压特征.  相似文献   

4.
断裂带物质组成、结构及其物理性质是理解断裂变形机制和地震破裂过程的基础和关键,断裂带地震(黏滑)和非地震(蠕滑)滑移行为不仅对了解地震活动性和山脉隆升过程具有重要意义,而且直接为防震减灾提供科学依据.我们以穿过龙门山映秀—北川和灌县—安县断裂带的汶川地震断裂带科学钻探(WFSD)岩心和地表出露的断裂带为研究对象,通过对断裂岩组成、结构、显微构造和钻孔物性测井数据进行分析研究,确定了龙门山逆冲断裂带滑移行为和物性特征,初步探讨了大地震活动性和有关断裂带的隆升作用:(1)映秀—北川断裂带倾向NW,浅部倾角~65°,发育的断裂岩厚约180~280 m,由碎裂岩、假玄武玻璃(地震化石)、断层泥和断层角砾岩组成.断裂带具有高自然伽马、高磁化率值、低电阻率、低波速等物理性质以及对称型破碎结构.断层泥普遍具有摩擦热效应的高磁化率值和石墨化作用特征,是古地震滑动的岩石记录.表明映秀—北川断裂带为经常发生大地震的断裂带,晚新生代以来类似汶川地震的大地震复发周期小于6000—10000年,具有千年复发周期特征.(2)灌县—安县断裂带倾向NW,浅部倾角~38°,发育的断裂岩厚约40~50 m,仅由断层泥和断层角砾岩组成,具有典型的"压溶"结构,表现出蠕滑性质.除压溶作用外,定向富集的层状黏土矿物和微孔隙的发育使断层强度变弱.断裂带具上盘破碎的非对称型破碎结构,除具低磁化率值特征外,其他物性与映秀—北川断裂带一致.(3)根据断裂岩厚度与断层滑移量相关经验公式关系,以及断层产状,粗略估算映秀—北川断裂带自中生代以来累积垂直位移量大于9 km,灌县—安县断裂带累积垂直位移量小于3 km.映秀—北川断裂带长期大地震产生的累积垂直位移量是龙门山隆升的主要贡献.  相似文献   

5.
汶川MS8.0级地震的发震构造为龙门山断裂带,地震地表破裂主要分布在其中的北川-映秀断裂和江油-灌县断裂上,尤其是沿前者发育了长达240 km左右的地表破裂带.通过对龙门山断裂带震后断层擦痕的测量,得到311条断层擦痕数据,利用由断层滑动资料反演构造应力张量的计算方法,得到研究区8个测点的构造应力张量数据,并获得了研究区构造应力场特征:区域现代构造应力场以近水平挤压为主,最大主应力方向(σ1)为76°~121°,平均倾角9°,应力结构以逆断型为主.受构造应力场及断层几何特征的影响,地表破裂呈现出分段性:映秀—北川段主要以NW盘逆冲为主,垂直位移明显;北川以北段为逆冲兼走滑,水平位移量与垂直位移量基本相当,或水平位移略大.  相似文献   

6.
汶川M_S8.0地震地表破裂带及其发震构造   总被引:178,自引:33,他引:145  
震后应急野外考察表明,2008年5月12日汶川MS8.0地震在青藏高原东缘龙门山推覆构造带上同时使北川-映秀断裂和灌县-江油断裂两条倾向NW的叠瓦状逆断层发生地表破裂。其中,沿北川-映秀断裂展布的地表破裂带长约240km,以兼有右旋走滑分量的逆断层型破裂为主,最大垂直位移6.2m,最大右旋走滑位移4.9m;沿灌县-江油断裂连续展布的地表破裂带长约72km,最长可达90km,为典型的纯逆断层型地表破裂,最大垂直位移3.5m;另外,在上述两条地表破裂带西部还发育着1条NW向带有逆冲垂直分量、左旋走滑性质的小鱼洞地表破裂带,长约6km。这一地表破裂样式是近期发生的特大地震中结构最复杂的一次逆断层型地表破裂,地表破裂的长度也最长。利用已有的石油地震剖面,结合余震分布和地表破裂带特征等资料构建的三维发震构造模型表明,龙门山推覆构造带现今和第四纪时期以地壳缩短为主,斜滑逆冲型地震表明青藏高原中东部的水平运动在华南地块与巴颜喀拉地块之间的龙门山推覆构造带上转化为地壳的缩短和隆升  相似文献   

7.
汶川Ms8.0级地震断层滑动机制研究   总被引:10,自引:3,他引:7       下载免费PDF全文
汶川Ms8.0级地震的发震构造为龙门山断裂带,地震地表破裂主要分布在其中的北川-映秀断裂和江油-灌县断裂上,尤其是沿前者发育了长达240 km左右的地表破裂带.通过对龙门山断裂带震后断层擦痕的测量,得到311条断层擦痕数据,利用由断层滑动资料反演构造应力张量的计算方法,得到研究区8个测点的构造应力张量数据,并获得了研究区构造应力场特征:区域现代构造应力场以近水平挤压为主,最大主应力方向(σ1)为76°~121°,平均倾角9°,应力结构以逆断型为主.受构造应力场及断层几何特征的影响,地表破裂呈现出分段性:映秀-北川段主要以NW盘逆冲为主,垂直位移明显;北川以北段为逆冲兼走滑,水平位移量与垂直位移量基本相当,或水平位移略大.  相似文献   

8.
汶川地震小鱼洞地区的地表破裂和同震位移及其机制讨论   总被引:1,自引:1,他引:0  
2008年5月12日在四川西部发生的汶川地震是一次以逆冲运动为主,兼有右旋走滑运动的斜滑型地震,形成了有史以来最长、最复杂的地表破裂之一.其中,很多复杂现象到目前为止还没有得到很好的解释或一致的认识,如小鱼洞地区出现的NW走向的小鱼洞断裂,在小鱼洞以北出现的2条相距llkm的平行断裂同时破裂的现象等.通过在小鱼洞地区的详细野外调查,获得了详细的地表破裂分布及同震位移分布,在此基础上对小鱼洞地区地表破裂的机制进行了分析.结果表明,造成上述复杂地表破裂的根本原因是汶川地震的主断层北川-映秀断裂的产状变化,即北川-映秀断裂在小鱼洞以北向NW偏移约3.5km.其破裂机制是:1)北川-映秀断裂的右旋走滑运动在小鱼洞西侧的左阶挤压阶区引起的挤压隆升形成前冲断层,即小鱼洞断裂;2)由于北川-映秀断裂在小鱼洞以北向NW偏移3.5km,导致其断层面倾角变大,逆冲运动引起的断层上盘对下盘的挤压方向变化,结合右旋走滑引起的上盘对下盘的侧向推挤,两者共同作用突破了彭灌断裂,从而形成了2条相距llkm的平行断裂同时错动的现象.另外,文中建议应该重视北川-映秀断裂右旋走滑运动分量、断层产状变化以及断层上、下盘的岩性差异对汶川地震地表破裂过程及地表破裂分布的影响.  相似文献   

9.
2008年5月12日四川汶川Ms8.0地震是一条陆内活动逆断裂带最新活动的结果.地震震源断裂沿龙门山构造带中央断裂发生斜滑作用和沿前山断裂发生纯逆断裂作用,断裂产状前者陡后者缓,垂直位移前者大后者小,这是一条少见的具有右旋走滑特征的挤压性质双断坡破裂,它是深部斜滑断裂在上地壳脆性域发生应变分解的结果.地震地表破裂带的分段活动和位移分布、地震波反演、余震空间分布、主震和余震震源机制解都说明这一条活动断裂带的活动机制和震源断裂破裂机制的复杂性.北西向小鱼洞左旋走滑破裂带是调节北东向破裂带中缩短量不同的破裂段之间的捩断裂,但由于震源断裂西南段经受着强烈挤压,左旋走滑的小鱼洞断裂也具有明显的挤压分量.在中央断裂这一条走滑逆冲和逆走滑性质的断裂和破裂带中出现的走滑正断裂控制的沙坝沟槽是在一个特殊的构造和地貌条件下,由震源断裂滑动和重力共同作用的结果,重力作用加大了该段破裂的正断层型垂直位移量,它不能真正代表震源断裂的最大地表垂直位移.  相似文献   

10.
研究了2008年汶川大地震的发震构造龙门山构造带的北段,即北川-南坝-林庵寺断裂的地表破裂.通过黄家坝、桂溪、平通、南坝、石坎子等地的考察和测量,显示该段地表破裂沿断裂带连续分布,走向为N45°~65°E.垂直位错与水平位错比值从西南段黄家坝的2.8:1逐渐降低到北东段南坝、石坎子的0.9:1.地表破裂特征表明,断裂以右旋走滑分量为主,并具有较高的逆冲分量.余震分布表明,青川断裂与北川-南坝-林庵寺断裂之间可能存在隐伏活动断裂.  相似文献   

11.
Slip rate along the major active fault is an important parameter in the quantitative study of active tectonics. It is the average rate of fault slip during a certain period of time, reflecting the rate of strain energy accumulation on the fault zone. It cannot only be directly applied to evaluate the activity of the fault, the probabilistic seismic hazard analysis, but also important basic data for the study of geodynamics. However, due to the nonstandardized process of obtaining fault slip rates for a given strike-slip fault, the results could be diverse based on various methods by different researchers. In this review, we analyzed the main advances in the approaches to obtain fault slip rate. We found that there are four main sources affecting the final results of slip rate: the displacement along the fault, the dating of the corresponding displacement, the fitting of the displacement and corresponding dating results, and paleoslip analysis. The main advances in obtaining fault slip rates are based on improving the reliability of the above four main factors. To obtain a more reasonable and reliable slip rate for a given fault, it is necessary to select a suitable method according to the specific situation.  相似文献   

12.
A closed-form analytic solution for the displacement and stress field due to a trapezoidal type of nonuniform slip along a strike slip fault is obtained by following Steketee’s method of integration. A set of displacement and stress contours are plotted and compared with the corresponding cases of uniform slip. A possible explanation of the equidistance distribution of strike slip faults and its relation to the amount of slip and the dimensions of the fault are shown.  相似文献   

13.
We present the data of the laboratory experiments on studying the regularities of gradual transition from the stick-slip behavior to aseismic creeping on the interblock boundary. The experiments show that small variations in the material composition in the principal slip zones of the faults may cause a significant change in the fraction of seismic energy radiated during the dynamic unloading of the adjacent segment of the rock mass. The experiments simulate interblock sliding regimes with the values of the scaled kinetic energy differing by a few orders of magnitude and relatively small distinctions in the strength of the contacts and in the amplitude of the released shear stresses. The results of the experiments show that the slip mode and the fraction of the deformation energy that goes into the seismic radiation are determined by the ratio of two parameters—the stiffness of the fault and the stiffness of the enclosing rock mass. An important implication of the study for solving the engineering tasks is that for bringing a stressed segment of a fault or a crack into a slip mode with low-intensity radiation of seismic energy, the anthropogenic impact should be aimed at diminishing the stiffness of the fault zone rather than at releasing the excessive stresses.  相似文献   

14.
General analytical expressions for the friction stress and state variable, based on a rate and state-dependent constitutive friction law proposed by Dieterich and Ruina, have been obtained as an explicit function of slip rateV or slip timet or slip displacement δ under the assumption that slip accelerationa is constant or piecewise constant. Properties of the solutions have been discussed, and reviewed, for uniformly accelerating (or decelerating) slip, the following.
  1. Frictional stress increases (or decreases) with increasing time, or slip rate, or slippage at the beginning of motion, until a maximum (or a minimum) value (when it exists) has been reached, then decreases (or increases), and finally approaches a special frictional state, namely a steady state, for which stress depends on instantaneous slip rate.
  2. The maximal value of frictional stress is dependent on accelerationa; the larger thea, the larger the magnitude of the maximum.
The energy expense ε needed to overcome the frictional stress has been estimated. And therefore the optimal value of acceleration for saving energy for a slipping mechanical system has been obtained. The energy release rateG for an abrupt rupture process of a crack or fault has been estimated.  相似文献   

15.
The propagation of slip along a pre-existing frictional plane is formulated for the faults containing interstitial fluid. When normal and shear stresses satisfy the effective frictional law, a frictional sliding occurs stably or unstably, depending on the inhomogeneities of the surface. For a slip to rapidly sweep the surface, the pore pressure of fluid must exceed the critical value that is related to the physical or geometrical irregularities of the surface. If this condition fails, stable sliding is expected, analogous to a seismic fault creep. This prediction makes the role of water in seismic faulting more clear.  相似文献   

16.
Slip nucleation during earthquakes is apparently analogous to rupture nucleation within an intact rock sample subjected to triaxial loading. The observations indicate that both these nucleation processes initiate within a relatively small volume and in both the slip propagates unstably along a quasi-planar surface. In both processes a single, pre-existing, shear fracture cannot nucleate the large-scale slip, and in both a ‘process zone' that includes several interacting fractures in a small volume are required to initiate the unstable slip. Both processes require rupture of intact rocks, generate complex fracture geometry, and are associated with intense energy-release rate during slip. Recent observations and analyses are used to correlate rupture nucleation in laboratory tests with nucleation events of large earthquakes. It is proposed that earthquake nucleation occurs by the interaction among multiple fractures within a small volume that develops into unstable yielding of the healed fault zone.  相似文献   

17.
解孟雨  史保平 《地震学报》2016,38(4):590-608
本文首先根据Dieterich和Ruina提出的含速率和状态的摩擦定律(Dieterich-Ruina定律), 基于一维弹簧-滑块模型推导了地震复发周期的解析表达式, 然后将该近似解与数值模拟结果以及Barbot等的相关研究进行了对比分析. 此外, 本文还利用数值模拟与理论分析研究了断层周期和非周期演化的力学成因机制以及非地震滑移形成的另类力学机制, 并讨论了一维弹簧-滑块模型的优点及其局限性. 结果表明: ① 震后滑移和自加速/成核阶段的持续时间在整个演化过程中不能被忽略; ② 在修正后的复发周期模型中, 复发周期的长短除了与断层特征尺度、 作用于断层面上的有效正应力和远场加载速率相关外, 还受Dieterich-Ruina定律中摩擦参数的取值以及临界滑移距离的影响; ③ 当给定各个物理参数和几何参数时, 目前所得到的解析近似解可以很好地估计地震的复发周期, 其相对误差可小于5%; ④ 在断层演化过程中, 施加剪切应力加载会产生非周期的地震滑移, 而在自加速/成核阶段后期或震后滑移阶段早期, 施加较大的剪切应力加载, 则会出现非地震滑移.   相似文献   

18.
Measurements of charge separation in rock during stable and unstable deformation give unexpectedly large decay times of 50 sec. Time-domain induced polarization experiments on wet and dry rocks give similar decay times and suggest that the same decay mechanisms operate in the induced polarization response as in the relaxation of charge generated by mechanical deformation. These large decay times are attributed to electrochemical processes in the rocks, and they require low-frequency relative permittivity to be very large, in excess of 105. One consequence of large permittivity, and therefore long decay times, is that a significant portion of any electrical charge generated during an earthquake can persist for tens or hundreds of seconds. As a result, electrical disturbances associated with earthquakes should be observable for these lengths of time rather than for the milliseconds previously suggested.  相似文献   

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