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31.
通过对色尔腾山山前断裂乌句蒙口 -东风村段的遥感资料解释、野外地质地貌考察 ,并通过对重点地段的古地震探槽开挖 ,获得了该断裂段晚更新世晚期以来的垂直位移速率是 0 88~ 1 83mm a ,全新世中期以来的垂直位移速率是 0 89mm a。通过 2个大型探槽的开挖、古地震事件分析和相关堆积物的断代研究 ,以及用逐次限定方法分析整个断层段上的古地震事件 ,认定该断裂段上全新世以来发生了 5次古地震事件 :事件 1发生在距今 90 0 0± 130 0年 ,事件2发生在距今 6 5 0 0± 5 0 0年 ,事件 3发生在距今 5 5 70年左右 ,事件 4发生在距今 4 2 0 0± 30 0年 ,事件 5发生在距今 32 5 0± 2 5 0年。晚更新世晚期到距今 1万年之间 ,古地震事件很不完整。全新世以来的 5次古地震事件表现出一定的丛集特征。最早的一丛事件发生在距今 890 0年左右 ,第2丛发生在距今 6 5 0 0~ 5 70 0年之间 ,第 3丛事件发生在距今 32 5 0~ 4 2 0 0年之间。第 1丛与第 2丛古地震事件之间间隔为 2 4 0 0年左右 ,而第 2丛与第 3丛古地震事件之间仅间隔 15 70年左右。距今 32 5 0年以来 ,该断裂段上还没有发生过错断地表的地震事件 ,已经超出了古地震丛之间的重复间隔。因此 ,它是色尔腾山前活动断裂带上具备潜在危险的一个活动断裂段。  相似文献   
32.
目的:将电阻率层析成像应用于探测潜伏断层的研究中,本文发现了断层和地下水的一些基本电阻率分布特征,这对于工程物探意义重大,一般情况下,断层两侧具有不同的电阻率特征,但是,根据电阻率层析图像中的电阻率分布,通常难以区分断层和地下水层,这是因为两者不仅都具有低电阻率值,而且还具有非常相似的电阻率异常特征。资料和方法:运用电阻率层析图像的数据,电阻率层析图像中的断层会呈现如下特征:1)由于孔隙度的加大和地下水的存在,使得断层表现出高角度的低阻线性结构。它们既可以出现在浅部盖层中,也可以存在于深部基岩中,特别是在深部区域,它们尤为明显;2)它们还呈现出高角度的线性梯度带,在该梯度带两边的电阻率结构出现整体性的差异,通常情况下,正断层的上盘表现出低阻或/和班驳状的高阻和低阻扰动区,而下盘则为完整的高阻区,这与逆冲断层正好相反;3)与断层有关的电阻率异常区常常具有良好的大尺度水平连续性,并且可以追瞎异常区附近的精细电性结构。而地下水的电阻率特征为:1)如果没有裂隙,地表水所引起的低阻区非常浅,即使存在丰富的水源以及高孔隙度的砾岩和中粗砂。一般情况下,其底端深度不超过强风化区;2)地下水的电阻率值非常低,特别在高矿化度的地区。地下水,包括岩溶水和砂岩水,的电阻率总显示出局部水平延伸或/和面团状特征;3)地下水层的深度朝某个固定方向逐渐增加,并且其电阻率图像会随季节而变;4)一般情况下,在水下渗的地区,会出现降水漏斗,其上部为高阻,而下部为低阻,从而便形成了“Y”或“V”字型的典型结构。结果:利用上述的基本特征一般可以区分断层和地下水。结论:仅依靠电阻率层析图像,可能极难准确地区分断层和裂隙水,这是因为裂隙水不但可能具有高角度的低阻线性结构,而且在一定尺度上具有很好的水平连续性,还有,由于电阻率层析成像较差的垂直分辨率,难以精确确定断层的上端点位置,所以结合其它的物探手段如钻探和浅层地震勘探是非常必要的。  相似文献   
33.
34.
长江口海域新生代地层与断裂活动性初探   总被引:7,自引:1,他引:7  
长江口海域通过浅层人工地震勘察查明,新生代地层可分为5个地震层。分别为第四系、上新统、中新统上段、中新统下段及始新统。第三纪地层自东北向西南依次超覆、减薄尖灭,上部被第四纪地层不整合覆盖。沉积基底主要由晚侏罗世火山岩系及燕山晚期酸性小岩体构成,未发现早第三纪及晚白垩世断陷盆地。断裂构造很发育,按展布方向大体可归为北东、北西及近东西向3组,皆为正断层。前两者数量多、延伸长、断距大,与同区的航磁异常构架吻合。北东向断裂分段明显,西南段为第四纪断裂,中段为晚第三纪断裂,东北段为早第三纪断裂;而北西向断裂分段不很清晰。两者的垂直位移速率平均在0.015mm/a。本文对该海域有关的几个地质问题进行了讨论。  相似文献   
35.
沈军  李军  赵纯青  葛敏 《内陆地震》2003,17(1):66-73
根据在乌鲁木齐市拟建华凌地下停车场活断层探测与地震危险性评价工作,对通过乌鲁木齐闹市区的雅玛里克断裂进行了实验性探测。采用了浅层地震探测、地质雷达探测、地形测量和坑探剖面方法,对这些手段的适用性进行了初步分析和讨论。  相似文献   
36.
岩石断裂作用的复杂性和混沌动力学   总被引:1,自引:0,他引:1  
断裂是一个复杂的动力学体系,受到岩石结构、反应、流体迁移、应力、岩石变形和力学等多种地质因素和过程的耦合控制。本文建立了断裂体系的反应-输运-力学耦合动力学模型并编制了模拟程序。以湖南水口山矿区为例,通过动力学模拟表明不同地层岩性的断裂渗透率大小和演化特征存在显著差异,断裂作用促使岩石渗透率的空间非均匀性增强,从而有利于流体的局部汇聚和矿体的形成。断裂中压力随时间呈现出非周期振荡变化,反映了断裂演化的混沌特征。  相似文献   
37.
The 3-D seismic tomographic data are used together with field, core and well log structural information to determine the detailed 3-D architecture of fault zones in a granitic massif of volume 500×575×168 m at Mina Ratones area in the Albalá Granitic Pluton. To facilitate the integration of the different data, geostatistical simulation algorithms are applied to interpolate the relatively sparse structural (hard) control data conditioned to abundant but indirect 3-D (soft) seismic tomographic data. To effectively integrate geologic and tomographic data, 3-D migration of the velocity model from the time domain into the depth domain was essential. The resulting 3-D model constitutes an image of the fault zone architecture within the granitic massif that honours hard and soft data and provides an evaluation of the spatial variability of structural heterogeneities based on the computation of 3-D experimental variograms of Fracture Index (fault intensity) data. This probabilistic quantitative 3-D model of spatially heterogeneous fault zones is suitable for subsequent fluid flow simulations. The modeled image of the 3-D fault distribution is consistent with the fault architecture in the Mina Ratones area, which basically consists of two families of subvertical structures with NNE–SSW and ENE–WSW trends that displaces the surfaces of low-angle faults (North Fault) and follows their seismically detected staircase geometry. These brittle structures cut two subvertical dykes (27 and 27′ Dykes) with a NNE–SSW to N–S trend. The faults present high FI (FI>12) adjacent bands of irregular geometry in detail that intersect in space delimiting rhombohedral blocks of relatively less fractured granite (FI<6). Both structural domains likely correspond with the protolith and the damaged zone/fault core in the widely accepted model for fault zone architecture. Therefore, the construction of 3-D grids of the FI in granitic areas affected by brittle tectonics permits the quantitative structural characterization of the rock massif.  相似文献   
38.
Southern Okinawa Trough represents an early stage of back-arc rifting and is characterized by normal faulting and microearthquakes. Earthquake distribution and deep structure of fault was investigated to clarify active rifting in the southern Okinawa Trough, where two parallel grabens are located. A network of ocean bottom seismometers (OBSs) that displayed the hypocenters of 105 earthquakes were observed for a period of 4 days in southern-graben (SG). Most of the microearthquakes occurred in a cluster about 7 km wide, which on a cross-section striking N45°E dips 48° to the southwest. Relocated hypocenters, which are recorded by a local seismic network, show scattered distribution around the southern-graben. There are no remarkable surface faults in the southern-graben. On the other hand, the recalculation of hypocenter locations of 1996 earthquakes swarm recorded by a local seismic network suggests that the swarm is associated with normal faulting on the southern side of northern-graben (NG). Thus, the undeveloped southern-graben is located to the south of the developed northern-graben. Southward migration of rifting, which may be caused by migration of volcanism, could thus be occurring in the southern Okinawa Trough. The extension rate computed for the southern Okinawa Trough from the fault model of the northern-graben is 4.6 cm/year, which is 59–102% of the extension rate (GPS measurements). This result indicates that the majority of extensional deformation is concentrated within the center of the northern-graben in the Okinawa Trough.  相似文献   
39.
Mine development along a 15-mile (24 km) section of the Warfield Fault in Mingo County, West Virginia has broadened the geological understanding of the fault and its related structures. The fault has been exposed in two new road cuts, one in the northeast-trending segment at Neely Branch and one in the eastern east-trending segment at the head of Marrowbone Creek. Both exposures show a well-defined normal fault with a 45° to 55° N dip, juxtaposing sandstone/shale packages from the roof and the floor of the Coalburg seam. The fault is associated with a thin gouge zone, some drag folding, and parallel jointing. Its trace tends to run parallel to the crest of the adjacent Warfield Anticline. Based on underground mine development and detailed core drilling, the vertical offset along the fault plane ranges from a maximum of 240 ft (73 m) in the central part of the area near the structural bend to less than 100 ft (30 m) in western and eastern directions. The fault is located along the relatively steeply dipping (locally in excess of 25%) southern limb of the Warfield Anticline, and appears related to a late phase of extension involving folded Pennsylvanian strata. On a regional scale, the lithological variations across the fault do not suggest any appreciable strike-slip component.Underground room and pillar mines in the Coalburg seam north and south of the fault have been greatly impacted by the Warfield structures. Due to the combined (and opposite) effects of the folding and faulting, the northern mines are located up to 400 ft (125 m) higher in elevation than the southern ones. Overland conveyor belts connect mining blocks separated by the fault. The practical mining limit along the steep slopes toward the fault is around 15%. Subsidiary normal faults with offsets in the 5- to 15-ft (1.5–4.5 m) range are fairly common and form major roof control and production hurdles. Overall, the Warfield structures pose an extra challenge to mine development in this part of the Appalachian Coalfields.  相似文献   
40.
The inference of fault geometry from suprajacent fold shape relies on consistent and verified forward models of fault-cored folds, e.g. suites of models with differing fault boundary conditions demonstrate the range of possible folding. Results of kinematic (fault-parallel flow) and mechanical (boundary element method) models are compared to ascertain differences in the way the two methods simulate flexure associated with slip along flat-ramp-flat geometry. These differences are assessed by systematically altering fault parameters in each model and observing subsequent changes in the suprajacent fold shapes. Differences between the kinematic and mechanical fault-fold relationships highlight the differences between the methods. Additionally, a laboratory fold is simulated to determine which method might best predict fault parameters from fold shape. Although kinematic folds do not fully capture the three-dimensional nature of geologic folds, mechanical models have non-unique fold-fault relationships. Predicting fault geometry from fold shape is best accomplished by a combination of the two methods.  相似文献   
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