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1.
隐伏逆断层破裂扩展特征的实验研究及其地震地质意义   总被引:3,自引:1,他引:2  
通过模拟实验研究了逆断层活动过程中上覆沉积层的破裂扩展特征,采用投影条纹测试方法分析了沉积层表面离面(即垂直)位移场的演化过程。结果表明,在沉积层厚度和断层倾角一定的条件下,基岩中的逆断层逐渐向上扩展,并在沉积层表面围绕基岩断层上断点的投影线形成一个离面位移梯度带(即形变带),基岩断层的位移越大,沉积层中的形变带越宽、变形越强烈;但当断层扩展至沉积层表面后,形变带宽度将保持稳定,只是变形随断层位移增加而更集中。对于同样的基岩断层位移和断层倾角,沉积层厚度越大,受基岩断层控制的形变带越宽,即基岩断层的影响范围越大;当沉积层厚度超过某一临界值时,沉积层中会发育因隆起引起的表面拉张破裂。在沉积层厚度和基岩断层位移量一定的情况下,基岩断层倾角的增加将会使表面形变带的宽度减小,但会使变形破坏程度更强烈。实验结果意味着,临界断层位移、临界沉积层厚度以及断层倾角对于确定隐伏逆断层发震产生的地表变形和破坏特征具有重要意义。文中的研究结果有助于进一步认识汶川MS8.0地震的地表变形特征  相似文献   

2.
梅世蓉 《地震学报》1996,18(2):170-178
从华北37次M6.0地震前的地震活动图象异常,以及1954~1992 年首都圈地壳形变图象研究中,提炼出强震前的异常特征;对强震前的地震活动图象异常与地壳形变异常进行对比分析.结果发现:① 强震前出现地震活动的增强与地壳形变速率的增大;② 震前数年环绕强震震中出现孕震空区与形变空区;③ 在图象动力学参数方面都表现出信息维的减小,表明地壳形变局部化随着时间而增加,是反映强震孕育阶段的重要现象和参量.最后,应用非均匀介质中非均匀坚固体孕震模式,对强震前地震活动图象与地壳形变图象异常物理机制给予了统一解释.   相似文献   

3.
引言地球内部介质发生微小形变时,介质会显示出弹性性质。当介质元偏离其固有位置时,介质元会发生围绕其原始位置的振动这种振动在地球内部的传播称为地震波。地震波的传播现象与声波、电磁波有相似之处,但地震波的传播是基于地球介质的弹性性质。地震波又可分为体波和面波。体波在介质内部传播,在固体内传播的地震体波分  相似文献   

4.
中国大陆及邻区上地幔各向异性研究   总被引:7,自引:0,他引:7       下载免费PDF全文
为了深化对中国大陆及邻区上地幔介质形变强度和方向的空间变化图象、各向异性和剪切波分裂、各向异性以及应变、应变和构造过程关系的认识,我们以剪切波在分层各向异性介质中的传播理论为指导,以分裂剪切波观测为基础,借助数字化地震资料和高分辨率的信号处理技术,给出了对136次地震的分析结果,得到了20个台站下面的上地幔各向异性介质的变形强度和方向的空间变化图象;并结合已有研究结果,对中国大陆及邻区上地幔各向异性特性及其起源问题进行了讨论.   相似文献   

5.
从华北37次M≥6.0地震前的地震活动图象异常,以及1954~1992年首都圈地壳形变图象研究中,提炼出强震前的异常特征;对强震前的地震活动图象异常与地壳形变异常进行对比分析.结果发现:①强震前出现地震活动的增强与地壳形变速率的增大;②震前数年环绕强震震中出现孕震空区与形变空区;③在图象动力学参数方面都表现出信息维的减小,表明地壳形变局部化随着时间而增加,是反映强震孕育阶段的重要现象和参量.最后,应用非均匀介质中非均匀坚固体孕震模式,对强震前地震活动图象与地壳形变图象异常物理机制给予了统一解释.  相似文献   

6.
利用甘肃岷县漳县6.6级地震区所在的青藏块体东北缘地区的区域水准、GPS、流动重力和跨断层短测线等地形变监测资料,结合地质构造、动力环境和已往的研究结果,分析了不同类型资料反映的震前区域性地壳变形背景、断层形变异常特征和可能的机理.结果认为:(1)岷县漳县6.6级地震前西秦岭、六盘山等构造区不同程度地存在着GPS水平挤压闭锁高应变积累、垂直隆升异常高梯度带和重力升、降差异剧烈变化等中长期背景;(2)震前到震时发震断裂附近及其外围相关构造区域断层形变异常在空间和时间上的起伏波动变化显著,尤其是汶川地震以来的波动变化在一定程度上反映了与本区构造比邻的龙门山断裂带剧烈右旋错动对本区的影响,与本次岷县6.6级地震过程有关;(3)本区有地形变监测资料积累以来缺乏6级以上震例,虽然存在不同程度的中长期形变背景异常,但何时进入短期-短临阶段确实很难把握,需要不断积累总结和探索提高.  相似文献   

7.
照片说明     
封2封3封底l当木日阿地震形变带的特征。 a为一期;b为二期;c为三期;d为四期.:为四期形变带在河岸边形成滑塌现象。镜头向东南拍。2当木日阿第三期地震形变带的特征。 地裂缝中巳有较多充填物,并有草本植物生长.镜头向东南拍。3当木日阿第四期地震形变带的特征。 地裂缝未见充填物和草不植物生长。镜头向东南拍.1当木日阿西岸一期、二期地震形变带为后期冲、洪积扁掩埋特征。 A为形变带;B为冲洪积扇。镜头向南拍.2当木日阿第一期地震形变带土珑、土沟展布特征. 土沟中可见“石沟”发育(人)。镜头向东北拍.3当木日阿第二期地震形变带土垅、土…  相似文献   

8.
利用南北地震带及附近地区20 多年来的大地垂直形变资料, 结合区域地震活动资料, 初步分析归纳了大地形变时空分布与地震群体活动的关系。在此基础上, 进一步对南北地震带中南段之川滇菱形块体形变场中期动态演化图象与b 值等地震活动参数图象进行了综合对比分析, 研究了形变场动态演化所揭示的区域现今构造运动的时空差异与反映地壳介质结构特性的b 值的时空分布变化、强震前后地震非均匀度值分布变化以及地震空区等的关系。结果表明: 强震前区域形变场动态演化与地震活动参数的时空分布均具有一定的非均匀特征, 二者所反映的大区域应力场变化与介质结构的不均匀导致的强烈差异运动产生的应变能积累是强震孕育的主要原因。得出了一些利用大地形变场动态演化与地震活动参数图象相结合进行强震中期预测的有益结果。  相似文献   

9.
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   

10.
高锡铭 《地震学报》1984,6(3):304-312
水库蓄水后,水体质量荷载引起地基岩石介质产生静力学形变效应.发生地震的水库,由于震源区岩石介质扩容,也会引起地基岩石介质的形变.本文同时考虑了这两种效应.水体质量荷载的静力学形变总效应包括:荷载引起的地基岩石介质的静态弹性形变,质量引起的重力等位面形变以及静态弹性形变所引起的重力等位面形变.岩石介质扩容效应在一定阶段会引起地基岩石介质的膨胀隆起,这种隆起形变同样也引起重力场变化.采用上述模型分析了丹江水库的水准测量成果,确定了该地区地基岩石介质的 Lame 常数,分析了地面垂直形变与地震的关系,从而认为使用该模型分析蓄水后库区的地面的垂直形变,可以为预报水库区地震提取必要的信息.   相似文献   

11.
The 1995 Kobe (Hyogo-ken Nanbu) earthquake, M = 7.2, ruptured the Nojima fault in southwest Japan. We have studied core samples taken from two scientific drillholes that crossed the fault zone SW of the epicentral region on Awaji Island. The shallower hole, drilled by the Geological Survey of Japan (GSJ), was started 75 m to the SE of the surface trace of the Nojima fault and crossed the fault at a depth of 624 m. A deeper hole, drilled by the National Research Institute for Earth Science and Disaster Prevention (NIED) was started 302 m to the SE of the fault and crossed fault strands below a depth of 1140 m. We have measured strength and matrix permeability of core samples taken from these two drillholes. We find a strong correlation between permeability and proximity to the fault zone shear axes. The half-width of the high permeability zone (approximately 15 to 25 m) is in good agreement with the fault zone width inferred from trapped seismic wave analysis and other evidence. The fault zone core or shear axis contains clays with permeabilities of approximately 0.1 to 1 microdarcy at 50 MPa effective confining pressure (10 to 30 microdarcy at in situ pressures). Within a few meters of the fault zone core, the rock is highly fractured but has sustained little net shear. Matrix permeability of this zone is approximately 30 to 60 microdarcy at 50 MPa effective confining pressure (300 to 1000 microdarcy at in situ pressures). Outside this damage zone, matrix permeability drops below 0.01 microdarcy. The clay-rich core material has the lowest strength with a coefficient of friction of approximately 0.55. Shear strength increases with distance from the shear axis. These permeability and strength observations reveal a simple fault zone structure with a relatively weak fine-grained core surrounded by a damage zone of fractured rock. In this case, the damage zone will act as a high-permeability conduit for vertical and horizontal flow in the plane of the fault. The fine-grained core region, however, will impede fluid flow across the fault.  相似文献   

12.
基于2009—2014年渭河盆地及邻区GPS资料,利用Shen提出的连续形变场与应变场计算方法,获得渭河盆地及邻区的水平形变场及应变率场,结合构造地质、地震目录等资料对渭河盆地及邻区的现今地壳形变及构造特征进行研究,并得到如下结论:(1)鄂尔多斯地块南缘西段和东段GPS形变场变化差异明显,六盘山—陇县—宝鸡断裂带形变场以挤压变形为主,渭河盆地中部西安—咸阳地区的形变场呈现EW向挤压、SN向拉张特征;(2)主应变率、剪应变率、面应变率变化明显的区域位于鄂尔多斯地块西南缘的六盘山—陇县—宝鸡断裂带、渭河盆地中部的长安—临潼断裂与渭南塬前断裂以及韩城断裂与双泉—临猗断裂附近;(3)未来需要警惕六盘山—陇县—宝鸡断裂带、长安—临潼断裂与渭南塬前断裂以及韩城断裂与双泉—临猗断裂附近的地震危险性。  相似文献   

13.
The geometry of faults at seismogenic depths and their continuation into the ductile zone is of interest for a number of applications ranging from earthquake hazard to modes of lithospheric deformation. Teleseismic passive source imaging of faults and shear zones can be useful particularly where faults are not outlined by local seismicity. Passive seismic signatures of faults may arise from abrupt changes in lithology or foliation orientation in the upper crust, and from mylonitic shear zones at greater depths. Faults and shear zones with less than near-vertical dip lend themselves to detection with teleseismic mode-converted waves (receiver functions) provided that they have either a contrast in isotropic shear velocity (V s), or a contrast in orientation or strength of anisotropic compressional velocity (V p). We introduce a detection method for faults and shear zones based on receiver functions. We use synthetic seismograms to demonstrate common features of dipping isotropic interfaces and contrasts in dipping foliation that allows determination of their strike and depth without making further assumptions about the model. We proceed with two applications. We first image a Laramide thrust fault in the western U.S. (the Wind River thrust fault) as a steeply dipping isotropic velocity contrast in the middle crust near the surface trace of the fault; further downdip and across the range, where basin geometry suggests the fault may sole into a subhorizontal shear zone, we identify a candidate shear zone signal from midcrustal depths. The second application is the use of microstructural data from exhumed ductile shear zones in Scotland and in the western Canadian Shield to predict the character of seismic signatures of present-day deep crustal shear zones. Realistic anisotropy in observed shear fabrics generates a signal in receiver functions that is comparable in amplitude to first-order features like the Moho. Observables that can be robustly constrained without significant tradeoffs are foliation strike and the depth of the foliation contrast. We find that an anisotropy of only a few percent in the shear zone is sufficient to generate a strong signal, but that the shear zone width is required to be >2 km for typical frequencies used in receiver function analysis to avoid destructive interference due to the signals from the boundaries of the shear zone.  相似文献   

14.
利用2009—2011、2011—2013、2013—2015年GPS形变资料,借助最小二乘配置方法、位移与应变的偏导关系,计算获得北天山东部应变场的动态演化结果,重新认识北天山东段构造区的现今活动特征,探讨应变场三个周期空间分布特征与2016年呼图壁6.2级地震的内部联系。结果表明:(1)区域地壳运动速率与应变场强度在时间上表现为“弱-强-弱”的变化特征,主应变率以NNW或NNE向的主压应变为主,第一、三周期N-S向主压应变较小,约(1~2)×10-8/a,第二周期变化显著增强,约(1~6)×10-8/a,第三周期滑动速率显示北天山东段呈“强[(2.2±0.4) mm/a]-弱(不明显)-强[(3.0±1.0) mm/a]”的右旋走滑特征;(2)地震可能更易发生在面应变率场等值线四象限中心区域或正、负过渡区的高密度梯度带内部,这可能是地震孕育过程中利用GPS资料观测到的形变前兆;(3)强震更易发生在剪应变率(最大剪应变率)的高值区或边缘区;(4)相对于面应变率与最大剪应变率等应变场物理量,主应变率更适用于在块体运动方向与性质上给出解释。  相似文献   

15.
Using Shen’s method (Shen et al., 1996), deformations of the Earth’s crust in Azerbaijan were studied based on GPS measurements. For estimating the rate of deformation, we used the field of velocity vectors for Azerbaijan, Iran, Georgia, and Armenia that were derived from GPS measurements during 1998–2012. It is established that compression is observable along the Greater Caucasus, in Gobustan, the Kura depression, Nakhchyvan Autonomous Republic, and adjacent areas of Iran. The axes of compression/contraction of the crust in the Greater Caucasus region are oriented in the S-NE direction. The maximum strain rate (approximately 200 × 10?9 per annum) is documented in the zone of mud volcanism at the SHIK site (Shykhlar), which is marked by a sharp change in the direction of the compression axes (SW-NE). It is revealed that the deformation field also includes the zones where strain rates are very low approximating 5 × 10?9 per annum. These zones include the Caspian-Guba and northern Gobustan areas, characterized by extensive development of mud volcanism. The extension zones are confined to the Lesser Caucasus and are revealed in the Gedabek (GEDA) and Shusha (SHOU) areas, as well as in the zone located between the DAMO and PIRM sites (Iran), where the deformation rate amounts to 100 × 10?9 per annum. It is concluded that the predominant factor responsible for the eruption of mud volcanoes is the intensity of gas-generation processes in the earth’s interior, while deformation processes play the role of a trigger. The zone of the epicenters of strong earthquakes is correlated to the gradient zone in the crustal strain rates.  相似文献   

16.
新疆天山地区壳幔S波速度结构特征及变形分析   总被引:1,自引:0,他引:1       下载免费PDF全文
天山地区地质构造复杂,地震活动频繁,其壳幔变形和深部结构一直受到学者们的高度关注.然而,由于天山地区地震台站资料较少,致使壳幔变形研究结果与解释存在诸多争议.本研究利用在天山地区(40°N-46°N,78°E-92°E)新布设的11个流动宽频带地震台站和该地区39个固定台站的观测资料,采用接收函数与面波联合反演方法,获得了研究区地壳厚度及壳幔S波速度结构.反演结果显示天山地区(41.5°N-44°N,78°E-88°E)平均地壳厚度为56 km,塔里木盆地(40°N-41.5°N,79°E-90°E)、准噶尔盆地(44°N-46°N,82°E-90°E)和吐鲁番盆地(42°N-43°N,88°E-90°E)具有较厚的沉积层,地壳平均厚度为43 km、53 km和46 km,整体表现为天山厚、盆地相对较薄的特征;在研究区南天山的最高峰(42°N,80.5°E)及北天山的最高峰(43.5°N,86°E)附近,中下地壳存在较厚的低速层,我们认为在强烈挤压作用下低速、低强度的中下地壳强烈变形可能是导致该区域快速隆升的主要原因.在研究区中部,位于塔里木盆地与准噶尔盆地之间的天山地区,中下地壳及上地幔均存在低速层,且盆地莫霍面向天山倾斜明显.结合前人的研究成果推测,在南北向构造挤压应力作用下,塔里木盆地与准噶尔盆地发生了向天山造山带方向的双向壳幔层间插入俯冲.在研究区东部,塔里木盆地东北缘与天山东部接触带的地壳内没有明显的低速层,推测应处在早期挤压变形状态,该区域的壳幔边界为缓变的速度梯度带,可能与上地幔热物质侵入或渗透有关.  相似文献   

17.
变形局部化问题和地震成核问题,是构造变形机制与大地震研究中极其重要的问题.对走滑断裂的运动和走滑型地震而言,断裂枢纽运动是断裂带上变形局部化和地震成核孕育的条件,认识这一运动过程和机制是了解走滑断裂上地震孕育、发生机制的关键之一.本文在前人工作的基础上,以则木河左旋走滑断裂大箐断层为例,测量了大箐断层大箐梁子断头沟台地-五道箐盆地之间的构造和地貌变形,揭示了大箐走滑断层枢纽运动构造和地貌四象限分布的特点,并且在定量分析其枢纽运动的基础上,利用数值模拟方法,模拟了断裂的枢纽运动,结果表明,走滑断裂的枢纽运动表现出典型的掀斜特征,随着断层面倾角的减小,枢纽运动程度加深;随着断层面闭锁区面积的增大,枢纽运动明显受阻;发现在闭锁区及其附近存在一个应力集中区使得应力由外向内一直处于积累状态,反映了地震的成核过程.  相似文献   

18.
Field studies and seismic data show that semi-brittle flow of fault rocks probably is the dominant deformation mechanism at the base of the seismogenic zone at the so-called frictional-plastic transition. As the bottom of seismogenic fault, the dynamic characteristics of the frictional-plastic transition zone and plastic zone are very important for the seismogenic fault during seismic cycles. Granite is the major composition of the crust in the brittle-plastic transition zone. Compared to calcite, quartz, plagioclase, pyroxene and olivine, the rheologic data of K-feldspar is scarce. Previous deformation studies of granite performed on a quartz-plagioclase aggregate revealed that the deformation strength of granite was similar with quartz. In the brittle-plastic transition zone, the deformation characteristics of granite are very complex, temperature of brittle-plastic transition of quartz is much lower than that of feldspar under both natural deformation condition and lab deformation condition. In the mylonite deformed under the middle crust deformation condition, quartz grains are elongated or fine-grained via dislocation creep, dynamic recrystallization and superplastic flow, plagioclase grains are fine-grained by bugling recrystallization, K-feldspar are fine-grained by micro-fractures. Recently, both field and experimental studies presented that the strength of K-feldspar is much higher than that of quartz and plagioclase. The same deformation mechanism of K-feldspar and plagioclase occurred under different temperature and pressure conditions, these conditions of K-feldspar are higher than plagioclase. The strength of granite is similar to feldspar while it contains a high content of K-feldspar. High shear strain experiment studies reveal that granite is deformed by local ductile shear zones in the brittle-plastic transition zone. In the ductile shear zone, K-feldspar is brittle fractured, plagioclase are bugling and sub-grain rotation re-crystallized, and quartz grains are plastic elongated. These local shear zones are altered to local slip-zones with strain increasing. Abundances of K-feldspar, plagioclase and mica are higher in the slip-zones than that in other portions of the samples (K-feldspar is the highest), and abundance of quartz is decreased. Amorphous material is easily formed by shear strain acting on brittle fine-grained K-feldspar and re-crystallized mica and plagioclase. Ductile shear zone is the major deformation mechanism of fault zones in the brittle-plastic transition zone. There is a model of a fault failed by bearing constant shear strain in the transition zone:local shear zones are formed along the fractured K-feldspar grains; plagioclase and quartz are fine-grained by recrystallization, K-feldspar is crushed into fine grains, these small grains and mica grains partially change to amorphous material, local slip-zones are generated by these small grains and the amorphous materials; then, the fault should be failed via two ways, 1)the local slip-zones contact to a throughout slip-zone in the center of the fault zone, the fault is failed along this slip-zone, and 2)the local slip-zones lead to bigger mineral grains that are in contact with each other, stress is concentrated between these big grains, the fault is failed by these big grains that are fractured. Thus, the real deformation character of the granite can't be revealed by studies performing on a quartz-plagioclase aggregate. This paper reports the different deformation characters between K-feldspar, plagioclase and quartz under the same pressure and temperature condition based on previous studies. Then, we discuss a mode of instability of a fault zone in the brittle-plastic transition zone. It is still unclear that how many contents of weak mineral phase(or strong mineral phase)will control the strength of a three-mineral-phase granite. Rheological character of K-feldspar is very important for study of the deformation characteristic of the granitic rocks.  相似文献   

19.
The Erguna Fault runs along the east bank of the Erguna River in NE China and is a large-scale ductile shear zone comprising granitic mylonites. This paper reports on the geometry, kinematic indicators, and 40Ar/39 Ar biotite ages of the granitic mylonites, to constrain the structural characteristics, forming age, and tectonic attribute of the Erguna ductile shear zone. The zone strikes NE and records a top-to-the-NW sense of shear. A mylonitic foliation and stretching lineation are well developed in the mylonites, which are classified as S-L tectonites. Logarithmic flinn parameters(1.18–2.35) indicate elongate strain which approximates to plane strain. Kinematic vorticity numbers are 0.42–0.92 and 0.48–0.94, based on the polar Mohr diagram and the oblique foliation in quartz ribbons, respectively, suggesting that the ductile shear zone formed under general shear, or a combination of simple and pure shear. According to finite strain and kinematic vorticity analyses, the Erguna Fault is a lengthening-thinning ductile shear zone that formed by extension. The deformation behavior of minerals in the mylonites indicates that the fault was the site of three stages of deformation: an initial stage of middle- to deep-level, high-temperature shear, a post-stress recovery phase of high-temperature static recrystallization, and a final phase of low-temperature uplift and cooling. The 40Ar/39 Ar plateau ages of biotite from the granitic mylonites are 106.16 ± 0.79 and 111.55 ± 0.67 Ma, which constrain the timing of low-temperature uplift and cooling but are younger than the ages of metamorphic core complexes(MCCs) in the Transbaikalia-northeast Mongolia region. Using measured geological sections, microtectonics, estimates of finite strain and kinematic vorticity, and regional correlations and geochronology, we conclude that the Erguna Fault is an Early Cretaceous, NNE-trending, large-scale, sub-horizontal, and extensional ductile shear zone. It shares a similar tectonic background with the MCCs, volcanic fault basins, and large and super-large volcanic-hydrothermal deposits in Transbaikalia-northeast Mongolia and the western Great Khingan Mountains, all of which are the result of overthickened crust that gravitationally collapsed and extended in the Early Cretaceous after plate collision along the present-day Sino-Russia-Mongolia border tract.  相似文献   

20.
马胜利  马瑾 《地震学报》1988,10(1):90-97
在不同的温度、压力条件下进行了含石英和方解石断层泥标本的摩擦实验。结果表明,石英断层带的摩擦强度对压力的响应直到400℃都很明显,对温度的响应在高温(高于400℃)时才明显;方解石断层带的摩擦强度对温度很敏感,对围压的响应只在低温(200℃)时才明显;随温度升高,石英和方解石断层带均由粘滑转变为稳滑,但前者的转换界限在400℃到500℃之间,而后者在200℃到300℃之间。显微观察表明,上述差异归因于其具体变形机制的差别。   相似文献   

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