共查询到18条相似文献，搜索用时 218 毫秒
1.
五莲拆离断层带中石英韧性变形明显,在野外主要表现为条带状、拔丝状,显微镜下主要表现为多晶石英条带,发育亚颗粒旋转重结晶和膨凸重结晶,剪切带经历了中低温条件下的变形,变形温度为300～450℃。利用分形方法对石英颗粒边界的研究表明,发生动态重结晶的石英颗粒边界具有统计学意义上的自相似性和明显的分形特征,亚颗粒旋转重结晶石英颗粒分维数介于1. 260～1. 319之间,均值1. 276;膨凸重结晶石英颗粒的分维数为1. 217～1. 297,均值为1. 256;根据石英粒径估算出亚颗粒旋转重结晶和膨凸重结晶作用变形阶段的古差异应力,分别为7. 84～21. 58MPa和18. 51～56. 65 MPa;基于分维值计算的应变速率计算公式,获得亚颗粒旋转与膨凸重结晶石英颗粒的应变速率分别为10-8. 4～10-7. 7s-1、10-10. 5～10-9. 7s-1;基于石英流变率计算,亚颗粒旋转重结晶的石英应变速率介于10-12. 88～10-11. 73s-1之间,膨凸重结晶的为10-13. 72～10-12. 46s-1。本地区韧性变形的应变速率大于一般性韧性剪切带应变速率,可能与拆离断层带的快速拆离伸展作用有关。 相似文献
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华北克拉通基底花岗质片麻岩变形和流变学研究——以辽西寺儿堡地区为例 总被引：2，自引：0，他引：2
辽西寺儿堡镇新太古代花岗质片麻岩内发育的宏观、微观构造变形特征表明该地区曾遭受了强烈的韧性变形改造。花岗质岩石变形程度在初糜棱岩–糜棱岩之间,岩石经历了SWW向左行剪切作用改造。岩石中石英有限应变测量判别结果表明,构造岩类型为L-S型,为平面应变。岩石的剪应变平均值为1.43,运动学涡度值为0.788~0.829,指示岩石形成于以简单剪切为主的一般剪切变形中。此外,石英颗粒以亚颗粒旋转重结晶和颗粒边界迁移重结晶作用为主,长石颗粒塑性拉长,部分发生膨凸式重结晶作用;石英组构特征(EBSD)揭示石英以中–高温柱面滑移为主;石英颗粒边界具有明显的分形特征,分形维数值为1.151~1.201,指示了中高温变形条件。综合石英、长石的变形行为、石英组构特征以及分形法Kruhl温度计的判别结果,推断辽西寺儿堡镇新太古代花岗质片麻岩经历过480~600℃的中高温变形,其同构造变质相为高绿片岩相-低角闪岩相。花岗质岩石的古差异应力为10.62~12.21 MPa,估算的应变速率为10~(–11.67)~10~(–13.34) s~(–1),即缓慢的变形,可能记录早期中高温、低应变速率的韧性变形过程,反映华北克拉通基底中下部地壳变形特征。 相似文献
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4.
桐柏杂岩北界剪切带是桐柏—大别造山带发育的一条大型的左行走滑韧性剪切带,发育糜棱岩、超糜棱岩以及强直片麻岩等强变形岩石。通过对剪切带内岩石的矿物共生组合、剪切带的位移量计算、石英的分维数计算、石英颗粒的差异应力以及应变速率的估算等多种方法分析结果显示:桐柏杂岩北界剪切带的位移量为38.3~41.1km;动态重结晶石英颗粒边界统计数据的相关系数R均大于0.96,动态重结晶颗粒边界具有统计意义上的自相似性;分维数为1.207~1.302之间,从剪切带的核部向边部,颗粒粒径和分维值的变化是逐渐变大的。石英的分维值反映出石英的动态重结晶与剪切带密切相关,变质变形由剪切带核部向边部逐渐减弱。桐柏杂岩北界剪切带的差异应力值为23.583~46.983 MPa之间,应变速率为1.70×10~(-11)~9.74×10~(-11)s~(-1)。通过对比剪切带内动态重结晶石英颗粒的粒径、差异应力和应变速率可以发现,差异应力与应变速率表现出一定的正相关性,都随着从剪切带的核部到边部慢慢变小;而石英的粒径则与差异应力和应变速率表现出负相关性,从剪切带核部到边部,随着石英粒径的变大,差异应力和应变速率变小。差异应力越大,导致石英颗粒的受力强度越大,变形越强,表现出来的就是应变速率越强。从显微构造变形角度来研究认识该剪切带,对揭示桐柏—大别造山带的构造演化以及构造模型的建立有着重要的构造意义。 相似文献
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位于北喜马拉雅穹隆带东段的然巴构造穹隆外围发育环形韧性剪切带,带内岩石经韧性剪切形成各类糜棱状岩石。石英为带内变形岩中最为常见的造岩矿物,在不同的温度、应变速率下产生不同的显微构造,其中动态重结晶最为常见。重结晶新晶颗粒边界普遍具有锯齿状或港湾状结构,是应变和变形环境的天然记录。新晶粒分维几何统计分析表明:带内动态重结晶石英颗粒边界形态具有自相似性(1≤D≤2),表现出分形特征,分维数值为1.14～1.19,变形温度大约500℃。同构造变质环境属中——高绿片岩相;初步估算古应变速率可能低于10-9.5S-1;根据重结晶粒径估算变形古应力6.2～58.8MPa。 相似文献
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西藏阿里札达韧性剪切带特征及其X光岩组分析 总被引：1，自引：0，他引：1
文中简述了西藏阿里札达盆地的地质背景、区域地层和札达韧性剪切带的基本特征。采用X射线衍射法对札达韧性剪切带中的石英、方解石和白云母等三种矿物,进行了X光岩组分析,确定了韧性变形岩石的组构特征、韧性剪切带的属性和变形岩石的应变类型,以及韧性剪切带形成时的温压条件。研究表明,韧性变形岩石均具不对称组构,反映韧性带属于南盘(下盘)俯冲型韧性剪切带,韧性变形是在高温、高压、低应变速率条件下发生的,处于>10km的地壳深度,岩石应变类型以压扁应变为主。 相似文献
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劝农山地区位于长春市东南部,处于佳-伊断裂和西拉木伦河缝合带交汇处.详细野外调查发现,该区曾遭受强烈韧性剪切变形,剪切带内岩石普遍糜棱岩化,主要由下二叠统范家屯组（P1f）钙质糜棱岩与侵入其中的燕山期花岗质糜棱岩组成,变形程度处于初糜棱岩至糜棱岩之间,多具有糜棱结构.岩石应变类型主要为压扁型应变,偏一般压缩,为L=S型构造岩,指示其形成于挤压型剪切带的构造环境.多种宏微观韧性剪切变形标志,指示明显的左行剪切运动.电子探针方解石-白云石地质温度计、方解石和石英EBSD组构特征、方解石e双晶形态以及石英长石变形行为等均显示岩石具有低温塑性流变特点,变形环境不超过绿片岩相.剪切带内应变速率偏高,应变集中带应变速率最大,在10-6.95~10-8.89之间,远离强变形带应变速率在10-9.25~10-12.17之间,糜棱岩化作用过程中差异应力下限应大致为51.27~65.46 MPa,代表剪切带糜棱岩化作用为低温中等强度应变,在稍快的应变速率条件下形成.压溶扩散和双晶滑移为劝农山韧性剪切带变形初期的主要变形机制,随着递进变形,逐渐以双晶滑移和晶内滑移为主,递进变形晚期,局部强变形域内发生了粒间滑移.劝农山韧性剪切带形成与早白垩世中晚期伊泽纳崎板块NNW向高斜度斜向俯冲于欧亚大陆之下有关,是佳-伊断裂带左旋走滑事件的局部表现. 相似文献
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江南造山带东段皖赣相邻区璜茅-五城-屯溪韧性剪切带野外现象、室内显微构造特征表明其经历了较为强烈的韧性剪切变形。岩石经历了NNE向右行剪切改造,变质变形程度为初糜棱岩-糜棱岩阶段,少量达超糜棱岩阶段。结合石英普遍发育边界迁移重结晶、长石多以塑性拉长和少量膨凸重结晶的变形行为特征、石英C轴组构显示出中-高温柱面和菱面滑移为主、重结晶石英颗粒大小-频数及分形维数(1.1646～1.2007),Kruhl温度计测算,揭示了璜茅-五城-屯溪韧性剪切带以中高温位错蠕变变形为主,变形和糜棱岩化环境在450～600℃的中深地壳范围,相当于中高绿片岩相-低角闪岩相。同时,岩石变形的古差异应力为20.76～30.04 MPa,估算所得应变速率主要介于10~(-14)～10~(-11) s~(-1),指示了中高温、低应变速率的韧性变形条件。已有的变形年龄显示,该韧性剪切带为加里东构造事件产物,主要的动力来源与江山-绍兴断裂带发育的陆内俯冲作用主应力在远离造山带的转变相关。 相似文献
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阿尔金北缘大平沟韧-脆性变形带特征 总被引：3，自引：2，他引：1
大平沟韧-脆性变形带出露于紧邻阿尔金北缘断裂北侧的新太古界达格拉格布拉克群钾长片麻岩中,与阿尔金走滑断裂索尔库里段相距约50km。总体呈东西向展布,高角度向南倾斜,倾角65～85°。次级变形带呈北西西向-东西向波状起伏延伸。单个次级变形带规模一般长数百米,宽数十米。变形带内岩石的线理、面理构造发育,石英、钾长石矿物粒内变形效应明显,同构造变形的新生矿物绢云母比较发育。变形性质为韧-脆性压扭性构造变形,发育糜棱岩系列岩石,特别是含钾长石残斑的绢云母石英质糜棱岩最为常见。变形岩石组构显示石英以底面和近于底面滑移的方式发生变形,反映出是中-低温条件(250～350℃);有限应变测量显示岩石变形强度中等,应变椭球轴比为2.9～4.8;变形运动学特点为右行逆冲,变形主压应力方向为北北西向,最大差应力为59～61MPa。结合区域构造演化,作者认为该韧-脆性变形带是发生于早古生代板块碰撞的大地构造背景条件下,并反映了板块碰撞过程中基底岩块的变形特点。 相似文献
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根据我国东部煤田一些实例和高温高压变形实验模拟结果表明,含煤地层中石英C-轴组构普遍具有稀疏小圆环带型式,其环带轴具有显著的应力指向意义。稀疏小圆环带型式组构的形成与石英底面滑移系的运动有关,是点极密型式的过渡状态,与石英颗粒的塑性应变量较小有关。造成含煤地层中石英颗粒塑性应变量较小的原因,除构造变形强度较小外,还与岩石中普遍存在软弱矿物有关。软弱矿物的存在吸收了大部分塑性应变 相似文献
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We conducted axial compression and general shear experiments, at T = 900 °C and P = 1.5 GPa, on samples of banded iron formation (BIF) and synthetic aggregates of quartz, hematite and magnetite to investigate how dynamic recrystallization of quartz promotes strain localization, and the role of weak second phases (oxides) on the rheology and microstructural evolution of the aggregates. Experiments showed strain localization into oxide rich layers, and that the oxide content and oxide distribution are key factors for the strength of the aggregate. Only 2–10 wt.% hematite leads to pronounced weakening and increasing hematite content above ∼10% has only a minor additional effect. Where oxide grains are dispersed, the initial strength contrast with quartz induces stress concentrations at their tips, promoting high stress recrystallization-accommodated dislocation creep of quartz. Fine recrystallized quartz reacts with oxide, forming trails of fine reaction product (ferrosilite/fayalite) leading to the interconnection/percolation of a weaker matrix. The strength contrast between the quartz framework and these fine-grained trails promotes strain localization into micro-shear zones, inducing drastic strain weakening. Thus dynamic recrystallization of quartz promotes syn-deformational reactions leading to a microstructurally-controlled evolution of phase strength contrast. It results in a rheologic transition from load-bearing framework to a matrix-controlled rheology, with transition from S–C′ to S–C fabric with increasing strain. 相似文献
12.
Johanns P. Walzebuck Wolf v. Engelhardt 《Contributions to Mineralogy and Petrology》1979,70(3):267-271
Planar elements in quartz, produced by shock induced plastic deformation, have been investigated in four quartz-plagioclase veins contained in an amphibolite from the crystalline basement of the Ries Crater from the drill hole Nördlingen 1973.The crystallographic orientation of planar elements in quartz grains is similar in all four rocks ({10¯13} predominant, {0001} less frequent, {10¯12} and others still rarer), indicating an average shock pressure in the range between 150 and 200 kbar.The spatial density of planar elements as measured by the number of systems per shocked grain, the number of individual elements per shocked grain, or as ratio shocked: unshocked grains increases with increasing grain size. This grain size effect is supposed to be primarily a consequence of the heterogeneity of the stress field which produced a random distribution of local stress maxima and locally restricted areas of plastic quartz deformation in the rock. The probability that planar elements develop within one individual grain increases, therefore, with increasing grain size.In one leucosome in which the quartz grains were randomly oriented planar elements parallel to {10¯13} cluster in a stereographic projection within one belt. It is supposed that the pole of this belt indicates the direction in which the shock front passed through the rock. 相似文献
13.
The mechanical properties and microstructures of mixed kaolinite/ quartz fault gouge have been studied by means of triaxial tests, wherein a 1 mm thickness of fault gouge was sheared between rigid, sintered alumina sliders. Test conditions ranged up to 200 MPa confining pressure, 175 MPa pore water pressure and temperatures to 600°C. Constant displacement rate tests were carried out at 5×10-4 mm s-1, and the stress relaxation technique was used to access a wide range of lower displacement rates down to 10-10 mm s-1. The effects of different ratios of clay: quartz were studied, and some experiments were cafried out using crushed Tennessee sandstone gouge and pre-faulted cylinders of Tennessee sandstone. Deformation-induced microstructures were studied by optical, scanning and transmission electron microscopy, and mineral chemistry changes were identified using EDS analysis in the STEM. The most important factor determining the strength of these gouges is effective confining pressure, and the effective stress law was obeyed at all test conditions. Increasing the proportion of quartz in the gouge slightly increases the strength, as does increase of temperature. Under all test conditions the gouges deformed by strain-hardening stable sliding. At 2 mm displacement the friction coefficient is similar to that for rock and rock sliding (μ= 0.85). Over wide ranges of strain-rate and temperature the strength of these gouges is little affected if the effective pressure is high, but strength drops rapidly with decreasing strain-rate if effective pressure is low (or if pore water pressure is high). Reloading of the gouge after stress relaxation at high temperatures demonstrated hardening arising from hydrothermal cementation during stress relaxation, which led to sudden rupture of the cemented gouge. This phenomenon may be responsible for cyclic rupture of natural faults. New mineral phases were produced in these experiments only at 600°C. At 400°C, anticipated production of pyrophyllite from kaolinite plus quartz was not found, but recrystallization of kaolinite is believed to have occurred and evidence of healing of cracks in quartz was seen. Microstructural studies revealed the ubiquitous development of P and R1 foliations and other features, which are identical to those found in natural clay-bearing fault zones. Microstructural evolution is associated with the strain-hardening, and apparent hardening is strongly associated with the stress path during loading. 相似文献
14.
Crystalline rocks from breccias of the Ries basin, Germany, contain highly deformed quartz. Various planar deformation structures could be observed and classified into five different types: (1) Decorated planar elements, (2) Non-decorated planar elements, (3) Homogeneous lamellae, (4) Filled lamellae, (5) Planar fractures. All these structures are parallel to crystallographic planes: {10¯13}, {10¯12}, {10¯11}, {0001},{11¯21}, {11¯22}, {21¯31}, {51¯61}, {10¯10}. The most typical and most abundant planar structures are decorated and nondecorated planar elements parallel to {10¯13} and {10¯12}. Planar fractures are parallel to {0001} and {10¯11} and form at lower stress levels, probably earlier than the planar elements.Quartz containing planar elements, especially of the non-decorated type, has lower density, index of refraction and birefringence than normal quartz. This quartz is apparently a mixture of an amorphous phase and crystalline quartz, the amount of which can be calculated using average density or refractive index.Comparison of planar quartz structures found in tectonites and those produced artificially under static or dynamic high pressure conditions demonstrates that Ries quartz closely resembles deformed quartz recovered from shock wave experiments. The planar structures found in Ries quartz have been formed by shock wave actions with peak pressures in the 100–400 kbar range.Planar elements are explained to be traces of gliding processes during shock loading visible due to the fact that a high pressure phase (stishovite and/or a stishovite-like glass phase) has been produced along the glide planes. Upon pressure release most of the high pressure phase was transformed into an SiO2-glass (diaplectic glass).In comparison with experimental data the amount of residual crystalline quartz as well as type and orientation of planar structures in the quartz grains are clues to estimate the peak pressures responsible for these deformations. Shock waves with peak pressures exceeding about 400 kbar completely transform quartz into diaplectic SiO2-glass. 相似文献
15.
河南桐柏老湾金矿床和花岗岩的年龄及其意义 总被引：19，自引：0，他引：19
通过老湾金矿床矿石中石英和花岗岩中的 主要造岩矿物石英、钾长石的40Ar/39Ar定 年,获得成矿年龄为91.5±1.0Ma,成岩期高温坪年龄为104.1±1.0Ma～108.9±0.3Ma,等 时线 年龄为102.8±0.1Ma～108.7±0.1Ma,因此认为成岩成矿具同时性。结 合 秦岭-大别造山带的演化历史,提出老湾金矿床和老湾花岗岩均形成于燕山晚期,成矿略晚 于成岩,构造应力环境为挤压向伸展转化的过渡期或以张应力为主的构造体制。 相似文献
16.
西华山钨矿床晶洞中水晶与黑钨矿流体包裹体显微测温与特征元素测定 总被引：2，自引：0，他引：2
摘要：西华山钨矿床晶洞中水晶与黑钨矿以及晶洞外部块状石英与共生黑钨矿中流体包裹体对比研究结果表明,后期应力作用和流体改造是造成共生石英与黑钨矿包裹体均一温度出现重大差异的主要原因。一般来说,在后期应力作用和流体改造下,黑钨矿有较好的稳定性,能较好地保存原生包裹体和较少出现次生包裹体,而与之共生石英中的原生包裹体几乎破坏殆尽,现在所看到的包裹体绝大部分是后来形成的次生包裹体,且很难确切区别原生与次生关系。当后期应力作用和流体改造很微弱时,石英中可保存较多原生包裹体,并且原生与次生关系较易区分。当完全未受应力作用改造时,共生石英(水晶)与黑钨矿中都只有原生包裹体,其Th值和盐度值基本相同或完全一致,且石英(水晶)流体包裹中富含W、Mn、Fe等成矿元素,表明石英与黑钨矿是由同一流体在相同时间和相同条件下沉淀的。鉴于一般金属矿床皆在一定程度上经受了后期应力作用和流体改造,因此在有关流体包裹体研究中应该结合不透明矿物进行全面对比,并且切实加强岩相学研究。 相似文献
17.
《Tectonophysics》1999,301(1-2):21-34
In order to clarify deformation mechanisms and behaviours of quartz in a low-temperature regime in the earth's crust, microstructural analyses, particularly on kink bands have been carried out for quartz veins moderately deformed under subgreenschist conditions. Both the dominance of subbasal deformation lamellae and geometry of kink bands suggest that basal (0001) slip was the sole active slip system in the deformed quartz. On a morphological basis, kink bands in the quartz were classified into two types: type I is characterized by conjugate and narrow bands with angular hinge zones, and type II by a wide monoclinal band. Dynamic analyses using deformation lamellae and kink bands have revealed that type I kink bands were formed in grains with basal plane (sub-)parallel to the compression axis, whereas type II kink bands were formed in grains with basal planes inclined to it. Using a numerical model of kinking of elastic multilayers modified after Honea and Johnson (Tectonophysics 30, 197–239, 1976), changes of the level of yielding stress for kinking and the width of kink bands as a function of the angle θ between the slip plane and the compression axis have been examined. The theory predicts that type I kink bands were formed at a higher stress level than type II kink bands, and hence occurrence of type I kink bands suggests that a significant strain hardening occurred in the deformed quartz veins. The theory also well explains the fact that the width of type I kink bands (θ=0 to 10°) is narrower by an order of magnitude than type II kink bands (θ=10 to 80°). 相似文献
18.
Rare earth element (REE) geochemistry on monomineral has been widely used in various fields of geosciences to reveal the origin
of ore-forming materials and fluid. Quartz are ubiquitous mineral in the Shihu gold deposit that is situated in central shear
zone of mesocenozoic Fuping metamorphic core complex in the middle-northern part of Taihang Mountains. Gold-bearing quartz
veins are their most important industrial orebodies. Rare earth element abundances in quartz from the Shihu gold mine, as
determined by laser ablation-indutively coupled plasma-mass spectrometry (LA-ICP-MS) analysis, are shown to be sensitive to
identify barren quartz and mineralized quartz. Amounts of REE concentrations in barren quartz and mineralized quartz are 97
× 10−9 and 85 × 10−9, respectively. The average (La/Yb)N and (La/Sm)N ratios for the barren quartz are 0.25 and 0.13, and the ratios for mineralized quartz are 0.28 and 0.19, respectively. There
is a pronounced positive correlation between (La/Yb)N and (La/Sm)N ratios. There is no obvious correlation between REE characteristics and sampling sites. The mineralized quartz show the most
pronounced negative Ce anomalies, whereas weak negative Ce anomalies are typical of barren quartz vein. A negative Eu anomaly
becomes more significant in mineralized quartz than barren quartz. δCe have a broadly positive correlation with δEu. Y/Ho
ratio of barren quartz and mineralized quartz are ranging from 2.14–28.75, and from 1.28–9.92, respectively. The REE characteristics
of quartz indicate that the ore-forming fluids of the gold deposit were derived from the deep fluid and its formation was
dually controlled by Precambrian metamorphic basement and Mesozoic granitoids. The results significantly enhance the usefulness
of quartz in tracing the sources of ore-forming fluid to discuss the genesis of the gold deposit, and as an indicator mineral
in mineral exploration in Taihang mountain region. 相似文献