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1.
Initially amorphous carbonaceous material becomes more crystalline with heating. The structural change depends not only on the maximum attained temperature but also the time‐scale of heating. Raman spectroscopy of natural samples that have been heated for time‐scales of 105 years or greater show that the degree of crystallinity has reached steady‐state. In contrast, laboratory studies show very little change in crystallinity of carbonaceous material (CM) after heating at 1000°C for a time of 3.5 weeks. Better constraints on the time‐scale for crystallization require experiments on time‐scales of years to thousands of years; such long time‐scales can only be derived from natural examples of CM‐bearing rocks that have been heated for a known length of time. Thermal modeling of contact metamorphism developed around a 13 m dike within the Akasaka Limestone in Gifu Prefecture shows the time‐scale of heating is of the order of 1–100 years. Raman spectroscopy reveals a significant increase in the crystallinity of the CM in a region within 3 m from the dike. A comparison between the temperature predicted for the contact aureole and the degree of crystallinity of the carbonaceous material shows that even close to the dike the CM has not reached steady‐state. This change began at over 550°C (modeled temperature) for a time‐scale of heating of a few years. Attaining steady‐state in the crystallization of CM under natural geological condition requires heating on time‐scales greater than about one hundred years. This study shows the utility of using natural laboratory studies to determine the kinetics of CM crystallization in rocks.  相似文献   

2.
Abstract To better understand heat generation and transfer along earthquake faults, this paper presents preliminary zircon fission-track (FT) length data from the Nojima Fault, Awaji Island, Japan, which was activated during the 1995 Kobe earthquake (Hyogo-ken Nanbu earthquake). Samples were collected of Cretaceous granitic rocks from the Ogura 500 m borehole as well as at outcrops adjacent to the borehole site. The Nojima Fault plane was drilled at a depth of 389.4 m (borehole apparent depth). Fission-track lengths in zircons from localities > 60 m distance from the fault plane, as well as those from outcrops, are characterized by the mean values of ≈10–11 μm and unimodal distributions with positive skewness, which show no signs of an appreciable reduction in FT length. In contrast, those from nearby the fault at depths show significantly reduced mean track lengths of ≈6–8 μm and distributions having a peak around 6–7 μm with rather negative skewness. In conjunction with other geological constraints, these results are best interpreted by a recent thermal anomaly around the fault, which is attributable to heat transfer via focused fluids from the deep interior of the crust and/or heat dispersion via fluids associated with frictional heating by fault motion.  相似文献   

3.
Yasu'uchi  Kubota  Toru  Takeshita 《Island Arc》2008,17(1):129-151
Abstract   The Median Tectonic Line (MTL) in southwest Japan, a major east–west-trending arc-parallel fault, has been defined as the boundary fault between the Cretaceous Sambagawa metamorphic rocks and Ryoke granitic and metamorphic rocks, which are unconformably covered by the Upper Cretaceous Izumi Group. The juxtaposition by faulting occurred after the deposition of the Izumi Group. Based on detailed fieldwork and previous studies, the authors reconstruct the kinematic history along the MTL during the Paleogene period, which has not been fully understood before. It is noted that although the strata of the Izumi Group along the MTL dip gently, east–west-trending north-vergent folds with the wavelength of ∼300 m commonly develop up to 2 km north from the MTL. Along the MTL, a disturbed zone of the Izumi Group up to 400 m thick, defined by the development of boudinage structures with the transverse boudin axis dipping nearly parallel to the MTL, occurs. Furthermore, east–west-trending north-vergent folds with the wavelength of 1–5 m develop within the distance up to 60 m from the MTL. The disturbed zone with the map-scale north-vergent folds along the MTL, strongly suggests that they formed due to normal faulting with a top-to-the-north sense along the MTL. Considering that the normal faulting is associated with the final exhumation of the Sambagawa metamorphic rocks, and its juxtaposition against the Izumi Group at depth, this perhaps occurred before the denudation of the Sambagawa metamorphic rocks indicated by the deposition of the Lower Eocene Hiwada-toge Formation. Dynamic equilibrium between crustal thickening at depth (underplating) and extension at shallow level is a plausible explanation for the normal faulting because the arc-normal extension suggests gravity as the driving force.  相似文献   

4.
We explore the fluvial response to faulting in three low‐gradient, sand‐bed rivers in south‐eastern Louisiana, USA, that flow across active normal faults from footwall (upstream) to hangingwall (downstream). We calculate sinuosity, migration rate and migration direction in order to identify anomalies spatially associated with fault scarps. In two of the rivers we model one‐dimensional steady water flow to identify anomalies in surface water slope, width‐to‐depth ratio, and shear stress. In each of these rivers there is one location where flow modeling suggests potential channel incision through the footwall, as indicated by relatively high surface water slopes and shear stress values. In one of these footwall locations, the river straightens and width‐to‐depth ratios decrease, likely contributing to higher surface water slopes and shear stress. This is in contrast to previous studies that have proposed increased sinuosity across fault footwalls and decreased sinuosity across hangingwalls. However, in two hangingwall locations we also observe relatively less sinuous channels. Other planform changes on the hangingwall include topographic steering of channels along and towards the fault and one example of an avulsion. The most notable anomaly in migration rate occurs on the hangingwall of a fault where a river has cut off a meander loop. Although fluvial response to faulting varies here, comparatively large and small channels exhibit similar responses. Further, Pleistocene fault slip rates are orders of magnitude lower than the channel migration rates, suggesting that faulting should not be a major influence on the fluvial evolution. Nonetheless, notable channel anomalies exist near faults, suggesting that recent fault slip rates are higher than Pleistocene rates, and/or that low‐gradient alluvial channels are more sensitive to faulting than previous studies have suggested. Rivers appear to be influenced by faulting in this setting, however background rates of meander loop cutoff may be just as influential as faulting. Copyright © 2015 John Wiley & Sons, Ltd.  相似文献   

5.
Field surveys and trench excavation investigations revealed that there were at least four large seismic events produced by slips on the Gosukebashi fault in the Holocene in the southeastern Rokko Mountains of Japan. The characteristics of deformed topographies and three-dimensionally excavated exposures show that this fault is a right-lateral strike–slip fault having an average slip rate of 1.0 mm/year, with a reverse displacement component. The principle indicators of past faulting events are: (i) termination of secondary faults; (ii) sedimentary deposits related to faulting; and (iii) injection veins of fault gouge related to seismic faulting in the fractured zone. Radiocarbon dates indicate that the events occurred pre-1660 BC , 1660 BC –220 AD , from ~ 30–220 to 600 AD and 15th century AD . The youngest event is probably associated with the large 1596 AD Keicho-Fushimi earthquake which occurred in the area around Kyoto and Kobe Cities. The second younger event is probably correlated with the 416 AD Yamato earthquake, which is the oldest historic earthquake in Japanese historic records. The results of trench surveys show that the horizontal displacement produced by an individual event is ~ 1.5 m, and the recurrence of seismic event intervals is ~ 1200 years in the Gosukebashi fault.  相似文献   

6.
An experiment is described in which a thin slab of granular material was shortened 70% in progressive pure shear between thick glass windows, at room temperature, 290 bars confining pressure, and 10?4 sec?1 strain-rate. The aim was to study the relation between microkinematic history and microstructural changes in the material. This was done by making transmitted light photomicrographs of the specimen in seven successive configurations, and reconstructing the six incremental displacement fields relating the seven configurations. The prominent structures formed are several conjugate faults, that correspond to discontinuities in the incremental displacement fields. Faulting is responsible, however, for only about half of the observed total shortening. The other half results from displacements without production of new planar features, termed flow. The photographs show that faulting and flow are synchronous. The faults thus rotate toward the principal direction of maximum elongation, and suitably oriented fault segments change in length while slip upon them continues. Slip continues on faults inclined at angles as low as 30° to the long axis of the total strain ellipsoid. Flow mechanisms include pore collapse and distortion, grain boundary sliding, slicing, and crystal plasticity. Pore collapse is seen in one case to play a role in accommodating displacements around the end of a fault. Experiments of this general type seem attractive for studying the relations between kinematic history and progressive structural changes in many kinds of materials, including materials that recrystallize, or melt, or undergo pressure solution during deformation. The implications of synchronous flow and faulting are discussed briefly.  相似文献   

7.
以2011年8月11日在伽师—阿图什交界处发生的5.8级地震为例,利用MODIS的LST产品数据,采用STL分解法有效地去除地表温度时空数据中的年变趋势及季节因素周期性的影响,对其余的残余项进行GESD异常检测,并分析2008年1月1日至2013年1月1日的LST异常及其他地震的关系数据,研究结果表明:(1)地表温度的变化具有明显的时空变化趋势;利用STL分解法可以看出震前存在明显的热红外异常,增温现象经历了"出现-扩大-分散增温-增温幅度达到极值-消失-发震"等几个阶段。(2)发震前四个月研究区周围存在明显的热红外异常,2月10日发震断层周围出现大面积异常,异常特征持续2个月后的4个月发震,峰值距发震时刻时间间隔较长。(3)余震分布与断裂带和热红外异常分布特征相关,震后大部分余震主要分布在主震发生的震前出现热红外异常的断裂带附近。(4)通过对比同地区相似震例发现,本次地震与2018年9月4日伽师县MS5.5地震的热异常特征有许多共同点,其中相同的峰值距发震时刻的时间间隔具有一致性,为震前热红外异常特征的归纳提供典型的参考信息。该次地震热红外异常显著,进一步验证了...  相似文献   

8.
青藏高原构造热演化的主要控制因素   总被引:23,自引:4,他引:23       下载免费PDF全文
从构造热演化的角度研究了青藏高原的形成模式,对形成机制中的两种主要假说:双地壳模型和叠瓦状模型进行了热模拟.在模拟时考虑了逆冲断层、均衡地壳抬升和沉积覆盖层对温度场的影响.结果表明,双地壳模型的热演化结果和实际观测资料明显不符;叠瓦状模型的结果在藏南地区能够较好地符合地球物理观测资料和解释地质构造运动.除较高的放射性元素含量外,断层的摩擦剪切热和沉积盖层热折射伴随地体的抬升侵蚀是喜马拉雅两条花岗岩带和反转的高温变质岩带的主要成因,并和现今上地壳水热活动有密切的关系.  相似文献   

9.
The relationship between the slip activity and occurrence of historical earthquakes along the Median Tectonic Line (MTL), together with that of the fault systems extending eastward has been examined. The MTL is divided into three segments, each containing diagnostic active faults. No historical earthquakes have been recorded along the central segment, although the segment has faster Quaternary slip rates compared with the other segments that have generated historical earthquakes. This discrepancy between earthquake generation and slip rate can be explained by a microplate model of southwest Japan. The microplate model also provides spatial and temporal coupling of slip on adjacent fault systems. In the context of this model, slip on adjacent faults reduces the normal stress on the MTL. Historical data and paleoseismic evidence indicate that slip on this segment occurs without significant strong ground motion. We interpret this as indicating anomalously slow seismic slip or aseismic slip. Slip on the central segment of the MTL creates transpressional regions at the eastern and western segments where historical earthquakes were recorded. Alternatively, the earthquakes at the eastern and western segments were triggered and concentrated shear stress at the edge of the segments resulted in postseismic slip along the central segment. The sequence of historical events suggests that the MTL characteristically does not produce great earthquakes. The microplate model also provides a tectonic framework for coupling of events among the MTL, the adjacent fault systems and the Nankai trough.  相似文献   

10.
The Raman spectra of carbonaceous material (CM) from 19 metasediment samples collected from six widely separated areas of Southwest Japan and metamorphosed at temperatures from 165 to 655°C show systematic changes with metamorphic temperature that can be classified into four types: low‐grade CM (c. 150–280°C), medium‐grade CM (c. 280–400°C), high‐grade CM (c. 400–650°C), and well‐crystallized graphite (> c. 650°C). The Raman spectra of low‐grade CM exhibit features typical of amorphous carbon, in which several disordered bands (D‐band) appear in the first‐order region. In the Raman spectra of medium‐grade CM, the graphite band (G‐band) can be recognized and several abrupt changes occur in the trends for several band parameters. The observed changes indicate that CM starts to transform from amorphous carbon to crystallized graphite at around 280°C, and this transformation continues until 400°C. The G‐band becomes the most prominent peak at high‐grade CM suggesting that the CM structure is close to that of well‐crystallized graphite. In the highest temperature sample of 655°C, the Raman spectra of CM show a strong G‐band with almost no recognizable D‐band, implying the CM grain is well‐crystallized graphite. In the Raman spectra of low‐ to medium‐grade CM, comparisons of several band parameters with the known metamorphic temperature show inverse correlations between metamorphic temperature and the full width at half maximum (FWHM) of the D1‐ and D2‐bands. These correlations are calibrated as new Raman CM geothermometers, applicable in the range of c. 150–400°C. Details of the methodology for peak decomposition of Raman spectra from the low to medium temperature range are also discussed with the aim of establishing a robust and user‐friendly geothermometer.  相似文献   

11.
Thermal models are developed and temperature-depth profiles computed to account for the development of sharply inverted metamorphic zonations and estimatedP-T conditions beneath deep-seated thrust faults, with particular reference to the metamorphism of the Pelona Schist-Vincent Thrust system of southern California.Models dependent only upon conductive redistribution of heat from an initially hot upper plate are inadequate to account for the observed temperature distributions and theP-T time constraints can only be satisfied if a total shear heating of 3 hfu or more occurs in the region of the thrusts. These heating rates are consistent with known rates of plate movement, shear stresses along major fault zones, and shear strengths of rocks.Petrological constraints indicate the likelihood of buffering of the maximum temperature attained by shear heating due to marked reduction of shear strengths of rocks upon increase of temperature and release of water during metamorphic dehydration reactions.These models may be of general applicability to inverted metamorphic zonations, notably those beneath obducted Newfoundland ophiolites, and are consistent with our present understanding of the thermal properties of the upper parts of subduction zones.  相似文献   

12.
Tetsuzo  Fukunari  Simon R.  Wallis 《Island Arc》2007,16(2):243-261
Abstract   The Median Tectonic Line (MTL) is a first-order tectonic boundary that separates the Sanbagawa and Ryoke Metamorphic Belts. Strike-slip movements on the MTL have been well documented by many workers. New field based structural studies in the Sanbagawa Belt close to the MTL reveal a large number of secondary faults and semibrittle shear bands indicating a top-to-the-north normal sense of displacement. The strikes of these shear zones and their spatial distributions suggest that development of these structures is related to movements on the MTL. These results imply that the MTL has a large-scale normal shear component on a regional scale that can help account for the exhumation of the Sanbagawa Belt. Our proposed history of the MTL can also account for changes in the geometry of folds in the Sanbagawa Belt.  相似文献   

13.
Using methods of discontinuous deformation analysis and finite element (DDA+FEM), this paper simulates dynamic processes of the Tangshan earthquake of 1976, which occurred in the northern North China where its internal blocks apparently interacted. Studies focus upon both the movement and deformation of the blocks, in particular, the Ordos block, and variations of stress states on the boundary faults. The Tangshan earthquake was composed of three events: slipping motions of NNE-striking major fault, NE-striking fault near the northeastern end of the NNE-striking fault, and NW-striking fault on the southeastern side of the NNE-striking fault. Compared with previous studies, our model yields a result that is more agreeable with the configuration of aftershock distributions. A number of data are presented, such as the principle stress field during the earthquake, contours of the maximum shear stress, the strike-slip deformation between blocks near the earthquake focus, time-dependent variations of slips of earthquake-triggered faulting, the maximum slip distance, and stress drops. These results are in accord with the earthquake source mechanism, basic parameters from earthquake wave study, macro-isoseismic line, observed horizontal displacement vectors, etc. The Tangshan earthquake exerted different influences on the adjacent blocks and boundary faults between them, thus resulting in differential movement and deformation. The Ordos block seems to have experienced the small-scale counterclockwise rotation and deformation, but its northeast part, bounded on the east by the Taihangshan and on the north by the Yanshan and Yinshan belts, underwent relatively stronger deformation. The Tangshan earthquake also changed the stress state of boundary faults of the North China, leading to an increase in shear stress and a decrease in normal stress in the NW-trending Zhangjiakou-Penglai fault through Tangshan City and the northern border faults of the Ordos block, and therefore raises the potential risk of earthquake occurrence. This result is supported by the facts that a series of Ms≥ 6 earthquakes took place at the northern margin of the Ordos block after the Tangshan earthquake.  相似文献   

14.
断裂带同震温度响应,可在震后钻孔测温中获得并识别,为发震断层摩擦特性与发震机制等基础研究提供了非常独特的思路和有效手段.集集、汶川及日本东北大地震后,实施了台湾车笼埔断层钻探项目(TCDP)、汶川地震断裂带科学钻探工程(WFSD)和日本海沟快速钻探计划(JFAST).钻孔测温结果表明:滑移面上下5~20m范围内存在温度正异常,这是同震摩擦生热所致,该机制已被广泛认识和接受;同时,距滑移面20~60m范围内也存在明显的温度负异常,但其成因机制几乎还未被真正关注和认识.虽然温度负异常峰值只有正异常峰值的1/4~1/3,但温度负异常分布范围却是正异常分布范围的3~4倍,即正、负温度异常区对应的总能量基本相当.因此,断裂带震后钻孔测温中的负异常及其成因不容忽视.在详细分析几种可能的同震温度负异常机制后(如岩层热物性分布差异、流体运移、表面自由能增大及同震应力释放),发现能在理论、实验及野外观测上都得到支撑的普适性机制只有同震应力释放.这可能是断裂带震后温度负异常的主要原因.  相似文献   

15.
通过利用发震区域的天体引潮力附加构造应力变化模型, 研究了2005年11月26日江西九江MS5.7地震发震构造与天体潮汐引力的关系, 并利用该模型结合美国国家环境预报中心多源综合温度数据资料, 分析了九江地震前后发震区域热异常在时空上的动态变化特征. 结果显示, 一方面, 在时间序列变化上, 孕震区热异常表现出的起始—消亡演变过程与岩石在应力加载下的形变—破裂过程相吻合. 无论近地表大气还是上附多层大气, 热异常主要集中在活动断裂带及其附近区域, 与构造断裂带分布相一致; 同时, 热异常从近地表到高空消失的垂向分布, 符合地面对大气加热导致大气升温→抬升→扩散→消亡的大气动力学基本特性, 表明构造运动是本次温度异常变化的主控原因. 另一方面, 热异常变化遵循引潮力(低值—高值—低值)的变化过程, 显示出天体引力对发震断层温度异常识别具有一定的指示意义以及引潮力可能对构造应力处于临界状态的发震断层具有诱震作用, 预示利用引潮力附加构造应力与热异常变化相结合研究短临地震预测具有一定价值.   相似文献   

16.
断层物质测年的热释光研究   总被引:4,自引:2,他引:4       下载免费PDF全文
计凤桔  马胜利 《地震地质》1994,16(2):167-175
断层物质TL测年的关键,是断裂运动产生的温压效应能否使断裂带内某些矿物原贮存的TL能量完全释放而“归零”。为此,进行了不同条件的高温、高压和位移速率变化等的模拟断裂运动的实验。结果表明,断裂运动产生的摩擦增温是使断层面上矿物TL强度减弱的主要因素。讨论了摩擦增温值与断裂运动时剪应力大小、断层泥厚度和断层位移间的关系,并得到了野外断层面上实际测试的证实。据此研究成果,还对小湾坝区F_7断裂的活动时代进行了测定  相似文献   

17.
地震的等震线不仅反映了地震的大小,而且也反映了地震断层过程的类型和破裂速度.单侧破裂的断层过程呈现出蛋型的等震线,而双侧破裂的断层过程呈现出椭圆的等震线,等震线的长轴与短轴之比对于破裂传播速度十分敏感.本研究利用理论等震线与观测结果相比较的方法,确定了1964年日本新地震、1983年日本海中部地震、1975年中国海城地震和1976年中国唐山地震的破裂传播速度、断层类型以及断层走向.得到的断层破裂速度是剪切波的0.7——0.9倍.这些值比用长周期地震波所确定的要稍大.产生这种差异的原因是:对烈度起主要影响的短周期地震波强烈地依赖于小尺度的断层不均匀破裂过程,以及局部的破裂传播的开始和终止;而由长周期波所得到的破裂速度却反映了在整个断层上破裂传播的平均过程.根据等震线图所得出的断层类型及断层走向与其它独立方法的结果相一致.这意味着本方法可以应用于推断某些历史地震的断层类型、破裂传播速度及破裂传播方向.   相似文献   

18.
Tectonically, the large-scale right-lateral strike-slip movement along the Red River fault zone is char-acterized at its late phase with the southeastward extension and deformation of the Northwestern Yunnan normal fault depression on its northern segment, and the dextral shear displacement on its central-southern segment. Research of the relations between stratum deformation and fault movement on the typical fault segments, such as Jianchuan, southeast Midu, Yuanjiang River, Yuanyang, etc. since the Miocene Epoch shows that there are two times dextral faulting dominated by normal shearing occurring along the Red River fault zone since the Miocene Epoch. The fission track dating (abbrevi-ated to FT dating, the same below) is conducted on apatite samples collected from the above fault segments and relating to these movements. Based on the measured single grain’s age and the con-fined track length, we choose the Laslet annealing model to retrieve the thermal history of the samples, and the results show that the fault zone experienced two times obvious shear displacement, one in 5.5 ± 1.5 MaBP and the other in 2.1± 0.8 MaBP. The central-southern segment sees two intensive uplifts of mountain mass in the Yuanjiang River-Yuanyang region at 3.6―3.8 MaBP and 1.6―2.3 MaBP, which correspond to the above-mentioned two dextral normal displacement events since the late Miocene Epoch.  相似文献   

19.
地震破裂过程的研究   总被引:1,自引:0,他引:1       下载免费PDF全文
研究震源力学模型的一个新方向是用动态扩展的剪切裂纹模拟地震破裂过程。本文利用裂端有塑性区薄层且断层面上有摩擦力的平面剪切裂纹错动模式来表示地震破裂过程,对运动方程和边界条件进行拉氏变换和傅氏变换,利用维纳-霍普(Wiener-Hopf)方法和卡格尼阿(Cagniard)方法得到了断层面上的位移和应力表达式。根据裂端附近的能量平衡条件,计算了地震破裂的平均速度和塑性区尺度,还讨论了断层面上的位错分布函数,并对某些前震地震波高频成分增多的现象提出了解释。在本文假定的参数条件下,地震破裂的平均速度c=0.72β,β是介质的剪切波速。塑性区尺度约为地震新断层总长度(包括塑性区)的12%。按本文的结果,由于破裂速度的增加,前震的震波初动半周期减小的异常幅度不会超过39%。  相似文献   

20.
断层活动不是孤立的,一条断层的活动可能影响其他断层,并引起这些断层的活动,这些相互作用的断层称为关联断层.本文利用卫星热红外信息以南北地震构造带为例,分析了关联断层活动的时空变化,所使用的信息是经过处理的地表亮温残差低频分量TLOW.结果表明,在一定时段内研究区一些断层间除地震活动表现出相互呼应关系外,其地表亮温残差低频分量TLOW曲线相似,相关系数高,说明热红外信息与地震信息共同反映一个地区断层的关联活动.此外,也存在单独由地表亮温残差低频分量TLOW相关表现断层关联活动的情形,即断层间无地震活动的呼应关系,但也存在TLOW曲线的相关性,同样显示关联断层的相互作用.对TLOW的时空过程分析表明,关联活动组合可随时间发生变化.例如,1988~1994年间红河断裂与澜沧-耿马断裂、金沙江断裂等构成关联活动组合,1994~1998年又与小金河断裂、安宁河-小江断裂构成关联活动组合,这样的时空变化过程可能是地壳应力场重新分配的反映.本文的研究结果证明,卫星热红外信息有望成为研究断层相互作用的一个新的独立物理量,并将对地震动力学和构造物理学的发展有重要意义.  相似文献   

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