首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 203 毫秒
1.
The SH wave spectra from some sequences of earthquakes of Kuril Islands and Chili regions, are examined following the dislocation model of seismic sources. We show by this way that, in a same sequence, it's difficult to correlate the magnitude with geometrical dimensions of the fault. We also make appear the persistence of the radiation, by developing for that, one method based on the comparison of the low frequency level with an isotropic quantity.

Résumé

On étudie le spectre des ondes SH, pour quelques séquences de séismes des Kouriles et du Chili, dans le cadre des modèles dislocatifs des sources sismiques. On montre ainsi que dans une même séquence, il est difficile de corréler la magnitude avec les dimensions géométriques de la faille. On met également en évidence la conservation de la radiation au cours d'une même séquence; on propose pour ceci une méthode, basée sur la comparaison des niveaux basses fréquences des spectres avec une quantité isotrope.  相似文献   

2.
The structure and energies of the cores of [100] and [001] screw dislocations in wadsleyite (β-Mg2SiO4) are calculated using a cluster-based combined elastic-atomistic method and a new parameterized interatomic potential model. For a core radius of 10 Å, core energies are found to be 2.5 and 4.4 eV/Å for the [100] and [001] dislocations, respectively. Both dislocations are associated with significant non-elastic displacement fields extending beyond the core with a radial component toward the dislocation line. The core of the [100] dislocation contains tetrahedrally coordinated magnesium, has a simple 2D structure and is spread parallel to (011) in a manner that suggests high mobility. In contrast, the core of the [001] dislocation has an extended and complex 3D structure involving the formation a large Si6O19 unit twisted around the dislocation line. This implies that movement of the [001] dislocation will be inhibited by the need to cleave Si–O bonds. These observations, combined with the anomalously low core energy of the [100] dislocation, explain the regular occurrence of [100] dislocations and very rare observation of [001] dislocations in experimentally deformed wadsleyite samples.  相似文献   

3.
西藏罗布莎地幔橄榄岩变形显微构造特征及其地质意义   总被引:1,自引:0,他引:1  
徐梦婧  金振民 《地质通报》2010,29(12):1795-1803
地幔橄榄岩是罗布莎蛇绿岩的主要组成成分之一,通过显微构造特征可对其变形特征进行分析,确定流变学参数,探讨地幔橄榄岩的变形历史。以蛇纹石化程度较低的二辉橄榄岩和方辉橄榄岩为研究对象,橄榄石位错特征研究显示,本区橄榄石主要发育了低温常见的直线型自由位错,局部可见位错弓弯、位错环、位错壁等高温位错,反映罗布莎地幔橄榄岩变形以低温塑性流变为主,局部经历了高温塑性流变,主导变形机制为位错蠕变。橄榄石自由位错统计结果表明,二辉橄榄岩中的橄榄石自由位错密度为4.422×107/cm2,方辉橄榄岩中的橄榄石为9.137×107/cm2,变形过程中所受差异应力分别为65MPa和93MPa。橄榄石和斜方辉石显微组构测量采用了电子背散射衍射技术(EBSD),分析结果表明,橄榄石均发育A型组构,为浅部地幔常见的组构类型,该结果与金刚石、柯石英等超高压矿物所指示的形成深度不一致。  相似文献   

4.
西藏东巧方辉橄榄岩的显微构造特征及其流变学意义   总被引:5,自引:2,他引:3  
西藏东巧地区蛇绿岩套中橄榄岩是青藏高原出露的为数不多的地幔岩体之一, 对于揭示该地区的上地幔流变学特征具有重要意义.报道了该地区方辉橄榄岩中橄榄石的位错显微构造特征, 估算了上地幔流变学参数.显微构造研究表明, 东巧方辉橄榄岩发育残斑结构, 橄榄石中位错组态类型比较丰富, 包括自由位错、位错壁(包括宽阔型和紧密型)、位错弓弯和位错网, 表明橄榄石的主导变形机制可能为位错蠕变.该区地幔岩变形大致分为2个阶段: (1) 地幔缓慢塑性流动变形, 形成宽阔型位错壁; (2) 蛇绿岩侵位过程中的变形, 产生紧密型位错壁.根据2种位错壁估算的流动应力平均值分别为3 9.3MPa (宽阔型)和113.9MPa (紧密型), 计算结果获得东巧地区上地幔流动速率为1.13× 10-12 ~ 2.95× 10-11s-1, 有效粘度为4.44×1017~ 1.16×1019Pa°s, 这些参数为东巧地区上地幔物理特征提供了流变学的约束条件   相似文献   

5.
研究了冀东马兰峪地区石英的TEM位错衍衬象。位错的形态及组态直接反映了地质样品的古应力及形成温度 ,可作为地质压力计使用 ,是将构造地质学的研究向定量化方向发展的重要手段之一。  相似文献   

6.
Omphacite grains from UHP eclogite of the Dabie Mountains in eastern China are elongated and show strong lattice preferred orientations (LPOs). Observations by the transmission electron microscopy (TEM) identified not only structures of plastic deformation occurring as free dislocation, dislocation loops and dislocation walls, but also bubbles of water present in the deformed omphacite. The bubbles attach to the dislocation loops which are often connected to one another via a common bubble. Using infrared spectroscopy (IR), two types of hydrous components are identified as hydroxyl and free-water in the omphacite. An analysis of deformation mechanism of microstructure in omphacite suggests that the mineral deformed plastically under UHP metamorphic conditions by dislocation creep through hydrolitic weakening.  相似文献   

7.
利用位错理论模型将遗传算法运用于断层三维滑动参数反演问题的求解,采用川西地区2004—2007年GPS观测数据对龙门山断裂带主要断层的三维滑动速率进行计算分析。结果表明:反演结果在量值上整体较小,与地质结果具有较好的一致性,走滑分量︱U1︱〈3.2 mm/a,倾滑分量︱U2︱〈1.54 mm/a,张开分量︱U3︱〈2.5mm/a,低滑动速率反映断层的闭锁及应力的积累及大地震发生的危险性;局部分量较地质结果偏大,反映实测GPS数据反演结果体现的是断层实时活动状态;遗传算法的全局收敛、不依赖初值等优点使结果更加稳定,而张开分量显示局部不规律性,表现出各子断层空间活动不均匀性。  相似文献   

8.
Facies and tectonic features have been analyzed in the area between Berchtesgaden and Funtensee (to the west of the Königssee) by use of modern methods (e.g. terrestrial photogrammetry, lineament analysis) and conventional geologic field work. Basing on the presentation of different examples, a model of the tectonic evolution is described consisting of six phases. They describe tectonical events from older Cimmerian to recent. It is shown that the manifold stress systems often reactivate older structures, a fact, which complicates the tectonik work significantly. Special emphasize is put to a strike-slip-fault system in 110° pointing to the recent principal stress component (140°) in the Northern Calcareous Alps.  相似文献   

9.
By the stress field’s reconstruction and the analysis of the distribution for the slickenside belts and the dike-hosting faults, the dominating left-lateral strike slip component is found for the Kolumbe Fault. This component is caused by the regional SES-NWN compression. The igneous rocks of the East Sikhote Alin volcanic-plutonic belt are considered as units synchronous with the regional displacement. Following the opinion of V.P. Utkin, the rift strike-slip-tension origin of these structures is suggested. Based on the structural-tectonic position of the volcanic rocks and the accompanying intrusive bodies and on the other geological data as well, several dislocation stages are distinguished in the Kolumbe Fault’s evolution. It is found that the dominating strike-slip motions along the main fault and its feathering faults changed to normal and reverse faulting deformations at the end of every stage.  相似文献   

10.
1970年通海地震的地震地质特征   总被引:3,自引:0,他引:3       下载免费PDF全文
张四昌  刘百篪 《地质科学》1978,13(4):323-335
一、前言1970年1月5日云南省通海、峨山、建水三县交界地区的曲江河谷发生了7.7级地震,震中位置是:东经102.6°;北纬24.1°,震源深度约为13公里。震中烈度10度强。  相似文献   

11.
橄榄石位错构造的扫描电子显微镜研究   总被引:1,自引:0,他引:1       下载免费PDF全文
利用扫描电镜的背散射电子图象(BEI)对玄武岩及金伯利岩所含幔源包体中橄榄石的缀饰位错进行了研究。实验结果表明,位错类型和颗粒边界图象清晰,又便于观察。这种观察位错的方法其分辨率比光学显微镜观察结果约高一个数量级。背散射电子图象位错方法特别适用于研究天然的和实验变形橄榄石的高位错密度和密集型边界,对于确定显微构造的定量参数也十分有利。  相似文献   

12.
由寒武系坚硬白云岩组成的汾河二库坝基开挖后,岩体沿顺层开裂面发生错位,错位波及几乎整个坝基,错距达1~7cm.本文对坝基岩体错位进行了分析研究,认为岩体错位是基坑开挖后地应力释放的结果。  相似文献   

13.
To understand the preservation of coesite inclusions in ultrahigh‐pressure (UHP) metamorphic rocks, an integrated petrological, Raman spectroscopic and focussed ion beam (FIB) system–transmission electron microscope (TEM) study was performed on a UHP kyanite eclogite from the Sulu belt in eastern China. Coesite grains have been observed only as rare inclusions in kyanite from the outer segment of garnet and in the matrix. Raman mapping analysis shows that a coesite inclusion in kyanite from the garnet rim records an anisotropic residual stress and retains a maximum residual pressure of ~0.35 GPa. TEM observations show quartz is absent from the coesite inclusion–host kyanite grain boundaries. Numerous dislocations and sub‐grain boundaries are present in the kyanite, but dislocations are not confirmed in the coesite. In particular, dislocations concentrate in the kyanite adjacent to the boundary with the coesite inclusion, and they form a dislocation concentration zone with a dislocation density of ~109 cm?2. A high‐resolution TEM image and a fast Fourier transform‐filtered image reveal that a tiny dislocation in the dislocation concentration zone is composed of multiple edge dislocations. The estimated dislocation density in most of the kyanite away from the coesite inclusion–host kyanite grain boundaries is ~108 cm?2, being lower than that in kyanite adjacent to the coesite. In the case of a coesite inclusion in a matrix kyanite, using Raman and TEM analyses, we could not identify any quartz at the grain boundaries. Dislocations are not observed in the coesite, but numerous dislocations and stacking faults are developed in the kyanite. The estimated overall dislocation density in the coesite‐bearing matrix kyanite is ~108 cm?2, but a high dislocation density region of ~109 cm?2 is also present near the coesite inclusion–host kyanite grain boundaries. Inclusion and matrix kyanite grains with no coesite have dislocation densities of ≤108 cm?2. Dislocation density is generally reduced during an annealing process, but our results show that not all dislocations in the kyanite have recovered uniformly during exhumation of the UHP rocks. Hence, one of the key factors acting as a buffer to inhibit the coesite to quartz transformation is the mechanical interaction between the host and the inclusion that lead to the formation of dislocations in the kyanite. The kyanite acts as an excellent pressure container that can preserve coesite during the decompression of rocks from UHP conditions. The search for and study of inclusions in kyanite may be a more suitable approach for tracing the spatial distribution of UHP metamorphic rocks.  相似文献   

14.
We show that naturally-deformed hematite from the Quadrilátero Ferrífero Province, Minas Gerais, Brazil, develops CPOs by dislocation creep, strongly influenced by basal plane parallel glide, even when this is not the favored slip system. Characterization of microstructure and texture, particularly intragranular misorientations, of naturally deformed hematite aggregates by EBSD allowed us to determine the importance of different slip systems, and confirm dislocation creep as the dominant deformation mechanism. Viscoplastic self-consistent (VPSC) models were constructed to constrain the slip systems required to operate for the observed CPO to develop, and its rheological implications. Changes in the CRSS ratio of hematite prism and basal slip systems and deformation regime lead to the development of distinct patterns of hematite crystallographic orientations. The basal slip-dominated simple shear model is the only one that can develop quasi-single-crystal CPO of the kind observed in highly deformed rocks from Quadrilátero Ferrífero. Comparison between naturally deformed hematite aggregates and VPSC models shows that CPO development of hematite is strongly influenced by a highly viscoplastic anisotropy through dislocation creep on hematite basal plane. Nonetheless, our results demonstrate that even the unfavorable slip systems should be regarded when the bulk rheology of mineral aggregates is evaluated.  相似文献   

15.
S. Santini  M. Dragoni  G. Spada 《Tectonophysics》2003,367(3-4):219-233
The 1964 Alaska earthquake was the second largest seismic events in the 20th century. The aim of this work is the use of surface deformation data to determine asperity and slip distributions on the fault plane of the Alaska earthquake: these distributions are calculated by a Monte Carlo method. To this aim, we decompose the fault plane in a large number of small square asperity units with a side of 25 km; this allows us to obtain plane surfaces with an irregular shape. In the first stage, each asperity unit is allowed to slip a constant amount or not to slip at all, providing the geometry of the dislocation surface that best reproduces the observed displacements. To this purpose, a large number of slip distributions have been tried by the use of the Monte Carlo method. The slip amplitude is the same for all the asperities and is equal to the average fault slip inferred from the seismic moment. In the second stage, we evaluate the slip distribution in the dislocation area determined by the Monte Carlo inversion: in this case, we allow unit cells to undergo different values of slip in order to refine the initial dislocation model. The results confirm the previous finding that the slip distribution of the great Alaska earthquake was essentially made of two dislocation areas with a higher slip, the Prince William Sound and the Kodiak asperities. Analysis of the post-1964 seismicity in the rupture region shows a strong correlation between the larger earthquakes (Mw≥6) and the distribution of locked asperities following the 1964 event, which can be considered as an independent test of the validity of the model. We do not find slip values higher than 25 m for any of the patches, and we determine two separate high-slip zones: one correspondent to the Prince William Sound asperity, and one (18 m slip) to the Kodiak asperity. The slip distribution connected with the 1964 shock appears to be consistent with the following seismicity in the region.  相似文献   

16.
Fine extinction bands (FEBs) (also known as deformation lamellae) visible with polarized light microscopy in quartz consist of a range of nanostructures, inferring different formation processes. Previous transmission electron microscopy studies have shown that most FEB nanostructures in naturally deformed quartz are elongated subgrains formed by recovery of dislocation slip bands. Here we show that three types of FEB nanostructure occur in naturally deformed vein quartz from the low-grade metamorphic High-Ardenne slate belt (Belgium). Prismatic oriented FEBs are defined by bands of dislocation walls. Dauphiné twin boundaries present along the FEB boundaries probably formed after FEB formation. In an example of two sub-rhombohedral oriented FEBs, developed as two sets in one grain, the finer FEB set consists of elongated subgrains, similar to FEBs described in previous transmission electron microscopy studies. The second wider FEB set consists of bands with different dislocation density and fluid-inclusion content. The wider FEB set is interpreted as bands with different plastic strain associated with the primary growth banding of the vein quartz grain. The nanometre-scale fluid inclusions are interpreted to have formed from structurally bounded hydroxyl groups that moreover facilitated formation of the elongate subgrains. Larger fluid inclusions aligned along FEBs are explained by fluid-inclusion redistribution along dislocation cores. The prismatic FEB nanostructure and the relation between FEBs and growth bands have not been recognized before, although related structures have been reported in experimentally deformed quartz.  相似文献   

17.
Transmission electron microscope (TEM) and high resolution transmission electron microscope (HRTEM) analyses have been performed on omphacite from ultra-high pressure (UHP) eclogites at the locality of Shima, Dabie Mountains, China. TEM reveals that the microstructures consist dominantly of dislocation substructures, including free dislocations, loops, tiltwalls, dislocation tangles and subboundaries. They were produced by high-temperature ductile deformation, of which the main mechanism was dislocation creep. Antiphase domain (APD) boundaries are common planar defects; an age of 470±6 Ma for UHP eclogite formation has been obtained from the equiaxial size of APDs in ordered omphacites from Shima, coincident with ages given by single-zircon U-Pb dating (471±2 Ma). HRTEM reveals C2/c and P2ln space groups in different parts of one single omphacite crystal, and no exsolution is observed in the studied samples, which is attributed to rapid cooling. It is suggested that the UHP eclogites underwent a long  相似文献   

18.
主要造岩矿物中位错分解及其流变学意义   总被引:1,自引:0,他引:1  
本文首次系统地综述了有关长石、橄榄石、石英和辉石等主要造岩物中位错分解研究的最新成果,探讨位错分解的流变学意义。为了方便读者,本文开始还扼要地介绍了一些位错分解的基本概念。  相似文献   

19.
走滑断层地震地表断裂位错估计方法研究   总被引:1,自引:0,他引:1  
赵颖  郭恩栋  王琼  刘智 《岩土力学》2013,34(5):1403-1408
为对一次地震中可能造成的地表断裂位错作出较准确的估计,采用拟静力弹塑性有限元方法,分别对覆盖土层为粉质黏土和黏土情况下,走滑断层引发的地震地表断裂进行了数值模拟分析。根据历史震害数据回归拟合的震级M与基岩位错 的关系式以及数值计算结果,建立了震级M与地表位错 的关系式。公式中考虑了土层厚度H对地表位错 的影响,而不仅仅局限于根据震级M的大小通过统计公式来估算地表断裂位错 。结果表明,走滑断层引发的地震地表断裂位错不仅与震级的大小有关,还与土层厚度和土层性质有关;在相同震级作用下,随着土层厚度的增加,地表位错逐渐减小;在相同震级和相同土层厚度下,上覆土层为粉质黏土时产生的地表位错要大于上覆土层为黏土时产生的地表位错;根据拟合的公式估计出不同震级情况下可不考虑走滑断层影响的临界覆盖土层厚度值,有助于提高活动断裂地震危险性评估工作的可靠性。  相似文献   

20.
宋旼 《冰川冻土》2007,29(3):482-486
与绝大多数材料遵循基于位错攀移的指数蠕变机制不同,多晶冰遵循基于位错滑移的指数蠕变机制,这种机制引起了冰川学家极大的兴趣.以前人的研究为基础,综述了冰中质子无序及质子点缺陷的形成过程,质子点缺陷对位错滑移影响的微观机理,以及多晶冰蠕变的微观机制.研究表明:冰晶体中的氢原子(质子)无序使得位错在滑移过程中形成质子点缺陷(D、L、H3O+和OH-缺陷),从而降低了位错的滑移速率.质子点缺陷的形成需要氢原子(质子)跃迁,其激活能大于水分子自扩散所需的激活能.同时,多晶冰的蠕变激活能与质子跃迁的激活能相当,而大于水分子自扩散所需的激活能,因此多晶冰的蠕变控制机制是位错滑移,而不是位错攀移.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号