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1.
流变学:构造地质学和地球动力学的支柱学科   总被引:12,自引:6,他引:6  
地球是一动态系统,其各层圈的构造运动归根到底就是多矿物复合岩石在各种物理条件(例如,温度、围压、差应力、应变速率、应变方式等)下和化学环境(例如,氧逸度和水含量)中的形变。流变学作为研究岩石力学性质和变形行为的科学,现已成为地球动力学和构造地质学的支柱学科。本文对国际上近年来岩石流变学的最新进展做些扼要的介绍,呼吁中国固体地学界加强流变学的研究,做出经得起时间淘洗、实践检验的原创性成果来,使中国的构造地质学研究迈进国际先进的行列。  相似文献   

2.
深部岩石力学性质及其在大陆构造变形过程研究中的作用   总被引:8,自引:4,他引:4  
在阐述了与深部岩石力学性质相关的岩石流变学基本模型的基础上,探讨了深部岩石力学性质对温度、压力和岩石化学组分等因素的依赖关系。根据目前对深部岩石力学性质的认识,讨论了岩石流变学在研究大陆构造变形过程中所起的重要作用。有关研究结果表明:在运用理论分析和数值模拟方法揭示大陆岩石圈中变形的动力学机制时,合理的选用深部岩石的流变学模型是必须考虑的一个重要因素。  相似文献   

3.
大陆下地壳麻粒岩的流变学研究进展   总被引:1,自引:0,他引:1  
大险下地壳麻粒岩的流变学研究可以解释地壳变形、壳幔物质交换以及岩石圈深部动力学过程等科学问题.前人通过研究各矿物的显微构造变形特征与变形机制,运用广义混合流变律探讨多矿物复合岩石的流变性质,结合水与流体对岩石变形强度的弱化作用,阐明在大陆下地壳变形环境下复矿麻粒岩的塑性变形和韧性流变性质.目前人们致力于对天然变形岩石和...  相似文献   

4.
超高压榴辉岩流变学研究   总被引:2,自引:0,他引:2  
大陆岩石圈和大洋岩石圈在成分、厚度和力学强度方面有明显的差别。因此,现有板块构造不完全适合于大陆构造。大陆地壳和上地幔流变学的综合研究是认识大陆构造最佳途径之一。流变学研究是大陆造山带几何学、运动学和动力学的桥梁。大陆岩石圈对构造作用、重力不稳定性和热结构的响应在很大程度上取决于岩石流变强度。岩石圈流变性质是岩石圈分层、构造复杂性和塑性流动的主导控制因素。超高压榴辉岩在地幔对流、壳-幔物质循环和俯冲带动力学起着重要作用。榴辉岩的流变性质和变形机制对于阐明大陆造山带和大陆深俯冲的动力学过程具有十分重要的意义。本文主要内容包括以下4个方面:(1)岩石流变学研究在地球动力学中地位和重要性;(2)回顾池际尚先生对岩石流变学实验的贡献;(3)近几年来超高压榴辉岩流变学研究成果;(4)国外岩石流变学实验研究发展态势和启示。  相似文献   

5.
岩石的结构、构造往往具有不均一性,因而表现出物理力学性质的各向异性。超声波技术就是通过研究岩石的各向异性来了解岩石的构造变形特征和微观构造。本文论述了这一方法的基本原理,介绍了检测方法,探讨了如何应用此法来确定主应变轴的空间方位和划分不同构造变形期次、确定岩石中微孔隙的排列方位和矿物定向组构、恢复古构造应力汤、区分原生和次生各向异性等。  相似文献   

6.
岩石组构记录了地壳形成与演化的关键信息,提取这些信息对分析和恢复地球动力学过程具有重要意义。磁化率各向异性(AMS)是一种重要的岩石组构方法,可以有效地揭示岩石的应变特征,分析其地球动力学过程,是研究构造变形性质以及应力作用方式的有效手段。本文在梳理AMS的研究历史、主要成果和最新进展的基础上,系统阐述了AMS的基本原理以及在剪切带的应用:①岩石组构具有复杂性,AMS作为一种间接组构手段受控于矿物的物理特性、含量以及变形变质等多方面因素;②AMS可以提供剪切带的运动学以及不同部位应变状态的信息;③对于剪切带,AMS主要受控于磁性矿物(矿物成分和粒度的变化导致全岩磁化率各向异性的变化)、构造变形强度(决定磁线理发展的重要因素)以及流体的作用(流体导致磁性矿物的类型与定向性的变化)。  相似文献   

7.
岩石圈流变学是大陆岩石变形的主导因素之一,是一种研究地球深部岩体变形的新方法。简要介绍流变学对大陆动力学研究的影响,并对当前流变学研究进展进行评述。岩石圈流变学在岩石圈地层、造山带和大型盆地动力学和动力学特征研究中的应用非常广泛。近年来,岩石圈流变学在脆-塑性转换、岩石流变含水性、“三明治”结构及岩石流变律等方面有重大进展。最后,指出目前岩石圈流变学还存在一些亟待解决的问题,如时间因素。  相似文献   

8.
刘贵 《地质力学学报》2020,26(2):175-186
构造变形与流体联合控制成矿作用的机制是矿床学界关注的热点问题之一。作为大陆岩石圈中的应变局部化带,剪切带中一般都渗透着大量流体,流体与岩石的相互作用及其化学效应和物理效应,导致了矿物化学不平衡和组分的迁移,引起岩石化学成分重新调整。文章通过对韧性剪切带内的流体作用、剪切带内的成分与体积变化、剪切变形与成矿模拟实验总结,讨论了剪切变形过程中的力学-化学作用、剪切构造应力和流体在构造成岩成矿过程中的行为。因此,要加强构造应力对温度、岩石物理性质、地球化学相平衡和水岩体系的相关参量方面影响的综合研究。   相似文献   

9.
侯泉林  LU Lucy Xi  程南南 《岩石学报》2021,37(8):2271-2275
构造地质学是地质学的核心基础学科,其发展方向是目前构造地质学家面临的挑战之一。本文从构造作用的本质出发,试图对构造地质学的发展方向进行思考。构造作用本质上是岩石和矿物对应力作用的响应,包括物理响应和化学响应,进而用数学方法进行表达:(1)物理响应主要表现为变形,包括脆性变形和韧性变形。岩石的力学性能决定了其变形特征。岩石圈力学性能在时间和空间上的不均一性一直是研究岩石圈变形行为的巨大挑战。需要结合野外观测、岩石力学和流变学研究,并借助多尺度模拟方法来建立不同时间尺度和空间尺度下岩石的变形行为和变形准则。(2)化学响应主要指构造应力作用下岩石和矿物发生化学变化的过程,即应力化学作用。变形变质作用、剪切带成矿作用、剪切带石墨化、应力生气和生烃等方面都可能存在应力化学过程,但其详细过程和反应机理还需要进一步探究。(3)运用数值模拟、量子计算对以上这些构造过程进行数学表达,也是构造地质学未来发展值得关注的方向。总之,构造地质学未来的发展方向应是与物理学、化学乃至数学等基础学科的深度融合。  相似文献   

10.
解读变形岩     
岩石变形既可以产生单个的宏观型构造,例如:破裂、断层、褶皱以及板块构造,也可以在岩石中产生中小尺度的构造形迹。变形岩石的组构取决于遭受变形的沉积岩或火山岩的特征或取决于矿物颗粒的或被改造的岩石碎屑的优选方位。   相似文献   

11.
岩石扩散蠕变及其地质意义   总被引:3,自引:1,他引:3  
总结了近十年来岩石扩散蠕变显微构造鉴别特征,研究方法的最新进展,矿物颗粒大小和流体(包括熔体和水)等是影响扩散蠕变的重要因素。扩散蠕变与位错蠕变和超塑性变形有密切关系,它的研究对大陆裂谷化过程,大陆碰撞带中岩石圈地幔强度弱化,中下地壳韧性剪切应变局限化以及与相变有关的矿物粒度细小化作用的分布有重要应用意义。  相似文献   

12.
赵中岩  方爱民 《岩石学报》2005,21(4):1109-1116
超高压变质岩是大陆深俯冲作用的产物。超高压变质岩在深俯冲和快速折返过程中,经历了长距离地构造搬运和构造力的作用。其构造变形主要集中在韧性剪切带中,并发生强烈地塑性流变。研究超高压变质构造岩的显微构造及其变形机制对于深入了解大陆壳岩石在深俯冲过程中的流变学行为有十分重要的意义,山东仰口的超高压韧性剪切带中榴辉岩质和花岗质糜棱岩记录了超高压变形的历史。在超高压条件下的稳定矿物绿辉石、多硅白云母、兰晶石和钾长石具有不规则波状消光、亚晶界、核幔构造和动态重结晶等显微构造特征,TEM 研究揭示了大量的位错构造,表明位错蠕变是其主要的变形机制。在花岗质糜棱岩中,金红石在刚性矿物的压力影中沉积,细粒的石榴石条带平行片理延伸,都说明超高压变形过程中有流体存在,流体助力的物质扩散迁移是又一个重要的变形机制。依据现有的流变学定律估算的流变应力应该在几十兆帕以上。  相似文献   

13.
Deformation mechanism maps for feldspar rocks   总被引:6,自引:0,他引:6  
Deformation mechanism maps for feldspar rocks were constructed based on recently published constitutive laws for dislocation and grain boundary diffusion creep of wet and dry plagioclase aggregates. The maps display constant temperature contours in stress-grain size space for strain rates ranging from 10−16 to 10−12 s−1.Two fields of dominance of grain boundary diffusion-controlled creep and dislocation creep are separated by a strongly grain size-sensitive transition zone. For wet rocks, diffusion-controlled creep dominates below a grain size of about 0.1–1 mm, depending on temperature, stress, strain rate and feldspar composition. Plagioclase aggregates containing up to 0.3 wt.% water as often found in natural feldspars are more than 2 orders of magnitude weaker than dry rocks. The strength of water-bearing feldspar rocks is moderately dependent on composition and water fugacity.For a grain size range of about 10–50 μm commonly observed in natural ultramylonites, the deformation maps predict that diffusion-controlled creep is dominant at greenschist to granulite facies conditions. Low viscosity estimates of 1018–1019 Pa·s from modeling postseismic stress relaxation and channel flow of the continental lower crust can only be reconciled with laboratory experiments assuming dislocation creep at high temperatures >900 °C or, at lower temperatures, diffusion creep of fine-grained rocks possibly localized in abundant high strain shear zones. For similar thermodynamic conditions and grain size, lower crustal rocks are predicted to be less than order of magnitude weaker than upper mantle rocks.  相似文献   

14.
In this contribution we present a review of the evolution of microstructures and fabric in ice. Based on the review we show the potential use of ice as an analogue for rocks by considering selected examples that can be related to quartz-rich rocks. Advances in our understanding of the plasticity of ice have come from experimental investigations that clearly show that plastic deformation of polycrystalline ice is initially produced by basal slip. Interaction of dislocations play an essential role for dynamic recrystallization processes involving grain nucleation and grain-boundary migration during the steady-state flow of ice. To support this review we describe deformation in polycrystalline ‘standard’ water-ice and natural-ice samples, summarize other experiments involving bulk samples and use in situ plane-strain deformation experiments to illustrate the link between microstructure and fabric evolution, rheological response and dominant processes. Most terrestrial ice masses deform at low shear stresses by grain-size-insensitive creep with a stress exponent (n ≤ 3). However, from experimental observations it is shown that the distribution of plastic activity producing the microstructure and fabric is initially dominated by grain-boundary migration during hardening (primary creep), followed by dynamic recrystallization during transient creep (secondary creep) involving new grain nucleation, with further cycles of grain growth and nucleation resulting in near steady-state creep (tertiary creep). The microstructural transitions and inferred mechanism changes are a function of local and bulk variations in strain energy (i.e. dislocation densities) with surface grain-boundary energy being secondary, except in the case of static annealing. As there is a clear correspondence between the rheology of ice and the high-temperature deformation dislocation creep regime of polycrystalline quartz, we suggest that lessons learnt from ice deformation can be used to interpret polycrystalline quartz deformation. Different to quartz, ice allows experimental investigations at close to natural strain rate, and through in-situ experiments offers the opportunity to study the dynamic link between microstructural development, rheology and the identification of the dominant processes.  相似文献   

15.
In high-grade (granulite facies) quartzofeldspathic rocks the progressive development of a fabric records contrasting deformation behaviour of quartz and feldspar. Feldspar has undergone deformation mainly by recrystallization-accommodated dislocation creep and produced smaller recrystallized grains progressively in the course of deformation. Quartz has not deformed solely by dislocation creep but also by a diffusion-controlled mechanism. Dislocation climb is important in the dislocation creep of quartz. In contrast to feldspar, quartz grains have not recrystallized into smaller grains at any stage of deformation. Rather, they have transformed initially to short monocrystalline ribbons and ultimately to long polycrystalline ribbons. This textural change of quartz is a continuous process and has taken place in the course of bulk textural change of the rocks during the deformation.  相似文献   

16.
The dominant flow mechanism in tectonic processes depends on the rheological properties of geological materials and the physical conditions prevailing during deformation. We have evaluated the relative importance of intercrystalline diffusion and intracrystalline creep in crustal deformation in terms of temperature and grain size.Oxygen isotope thermometry has been used to elucidate the thermal environment obtaining during deformation and contemporaneous metamorphism of Dalradian rocks from Southwest Scotland. The temperature and grain size data, applied in conjunction with microstructural criteria for evaluating independent mechanisms of steady-state flow, allow recognition of a low-temperature deformation regime dominated by intercrystalline diffusion, and a high-temperature regime dominated by dislocation processes.The transition between the fields of intercrystalline diffusion and dislocation creep for quartz and calcite of 100 Mm grain size occurs at about 450° C and about 300° C, respectively. These empirically derived results are consistent with the temperature intervals over which intercrystalline diffusion and dislocation creep, respectively, are predicted to be dominant at geologically reasonable strain rates, as derived from theoretically formulated deformation mechanism maps for quartz and calcite.Grain growth may play an important role in delimiting the higher-temperature boundary of the intercrystalline diffusion field. Intercrystalline diffusion is the only deformation mechanism that involves mass transfer over distances that are large in relation to the grain size. This result has important consequences for geochemical transport phenomena.  相似文献   

17.
Experimental deformation of partially melted granitic aggregates   总被引:16,自引:1,他引:16  
Abstract The effects of varying amounts of partial melt on the deformation of granitic aggregates have been tested experimentally at conditions (900°C, 1500 MPa, 10-4 to 10-6/s) where melt-free samples deform by dislocation creep, with microstructures approximately equivalent to those of upper greenschist facies. Experiments were performed on samples of various grain sizes, including an aplite (150 μm) and sintered aggregates of quartz-albitemicrocline (10–50 and 2–10 μm). Water was added to the samples to obtain various amounts of melt (1–15% in the aplite, 1–5% in the sintered aggregates). Optical and TEM observations of the melt distribution in hydrostatically annealed samples show that the melt in the sintered aggregates is homogeneously distributed along an interconnected network of triple junction channels, while the melt in the aplites is inhomogeneously distributed. The effect of partial melt on deformation depends an melt amount and distribution, grain size and strain rate. For samples deformed with ? 1% melt, all grain sizes exhibit microstructures indicative of dislocation creep. For samples deformed with 3–5% melt, the 150 μm and 10–50 μm grain size samples also exhibit dislocation creep microstructures, but the 2–10 μm grain size samples exhibit abundant TEM-scale evidence of dissolution-precipitation and little evidence of dislocation activity, suggesting a switch in deformation mechanism to predominantly melt-enhanced diffusion creep. At natural strain rates melt-enhanced diffusion creep would predominate at larger grain sizes, although probably not for most coarse-grained granites. The effects of melt percentage and strain rate have been studied for the 150 μm aplites. For samples with ? 5 and 10% melt, deformation at 10–6/s squeezes excess melt out of the central compressed region allowing predominantly dislocation creep. Conversely, deformation at 10-5/s produces considerable cataclasis presumably because the excess melt cannot flow laterally fast enough and a high pore fluid pressure results. For samples with 15% melt, deformation at both strain rates produces cataclasis, presumably because the inhomogeneous melt distribution resulted in regions of decoupled grains, which would produce high stress concentrations at point contacts. At natural strain rates there should be little or no cataclasis if an equilibrium melt texture exists and if the melt can flow as fast as the imposed strain rate. However, if the melt is confined and cannot migrate, a high pore fluid pressure should promote brittle deformation.  相似文献   

18.
Garnet (10 vol.%; pyrope contents 34–44 mol.%) hosted in quartzofeldspathic rocks within a large vertical shear zone of south Madagascar shows a strong grain‐size reduction (from a few cm to ~300 μm). Electron back‐scattered diffraction, transmission electron microscopy and scanning electron microscope imaging coupled with quantitative analysis of digitized images (PolyLX software) have been used in order to understand the deformation mechanisms associated with this grain‐size evolution. The garnet grain‐size reduction trend has been summarized in a typological evolution (from Type I to Type IV). Type I, the original porphyroblasts, form cm‐sized elongated grains that crystallized upon multiple nucleation and coalescence following biotite breakdown: biotite + sillimanite + quartz = garnet + alkali feldspar + rutile + melt. These large garnet grains contain quartz ribbons and sillimanite inclusions. Type I garnet is sheared along preferential planes (sillimanite layers, quartz ribbons and/or suitably oriented garnet crystallographic planes) producing highly elongated Type II garnet grains marked by a single crystallographic orientation. Further deformation leads to the development of a crystallographic misorientation, subgrains and new grains resulting in Type III garnet. Associated grain‐size reduction occurs via subgrain rotation recrystallization accompanied by fast diffusion‐assisted dislocation glide. This plastic deformation of garnet is associated with efficient recovery as shown by the very low dislocation densities (1010 m?3 or lower). The rounded Type III garnet experiences rigid body rotation in fine‐grained matrix. In the highly deformed samples, the deformation mechanisms in garnet are grain‐size‐ and shape‐dependent: dislocation creep is dominant for the few large grains left (>1 mm; Type II garnet), rigid body rotation is typical for the smaller rounded grains (300 μm or less; Type III garnet) whereas diffusion creep may affect more elliptic garnet (Type IV garnet). The P–T conditions of garnet plasticity in the continental crust (≥950 °C; 11 kbar) have been identified using two‐feldspar thermometry and GASP conventional barometry. The garnet microstructural and deformation mechanisms evolution, coupled with grain‐size decrease in a fine‐grained steady‐state microstructure of quartz, alkali feldspar and plagioclase, suggests a separate mechanical evolution of garnet with respect to felsic minerals within the shear zone.  相似文献   

19.
超高压榴辉岩中绿辉石组构和变形机制研究进展   总被引:2,自引:0,他引:2  
榴辉岩中绿辉石晶格优选方位(LPO)类型主要有S型(压扁型)组构、L型(收缩型)组构、L-S中间型组构、退火型组构,其中L型和S型组构是绿辉石在超高压岩石中最发育的组构类型.矿物组构的产生与变形机制密切相关,目前还无法解释绿辉石LPO产生和变化的原因.对天然绿辉石变形机制的最新研究进行了评述,包括位错蠕变产生变形绿辉石LPO的传统观点,以及扩散蠕变伴随晶体各向异性生长和空间群转换两种新观点.使用费氏台对大别山双河地区榴辉岩中的绿辉石组构进行了测量,并用电子背散射衍射技术(EBSD)对测量结果进行了验证.结合榴辉岩的显微构造和绿辉石组构特征对大别山双河超高压榴辉岩中绿辉石的变形机制进行了初步探讨,认为其变形机制以位错蠕变为主.  相似文献   

20.
It is now admitted that the high strength of the subcontinental uppermost mantle controls the first order strength of the lithosphere. An incipient narrow continental rift therefore requires an important weakening in the subcontinental mantle to promote lithosphere-scale strain localisation and subsequent continental break-up. Based on the classical rheological layering of the continental lithosphere, the origin of a lithospheric mantle shear/fault zone has been attributed to the existence of a brittle uppermost mantle. However, the lack of mantle earthquakes and the absence of field occurrences in the mantle fault zone led to the idea of a ductile-related weakening mechanism, instead of brittle-related, for the incipient mantle strain localisation. In order to provide evidence for this mechanism, we investigated the microstructures and lattice preferred orientations of mantle rocks in a kilometre-scale ductile strain gradient in the Ronda Peridotites (Betics cordillera, Spain). Two main features were shown: 1) grain size reduction by dynamic recrystallisation is found to be the only relevant weakening mechanism responsible for strain localisation and 2), with increasing strain, grain size reduction is coeval with both the scattering of orthopyroxene neoblasts and the decrease of the olivine fabric strength (LPO). These features allow us to propose that grain boundary sliding (GBS) partly accommodates dynamic recrystallisation and subsequent grain size reduction.A new GBS-related experimental deformation mechanism, called dry-GBS creep, has been shown to accommodate grain size reduction during dynamic recrystallisation and to induce significant weakening at low temperatures (T < 800 °C). The present microstructural study demonstrates the occurrence of the grain size sensitive dry-GBS creep in natural continental peridotites and allows us to propose a new rheological model for the subcontinental mantle. During dynamic recrystallisation, the accommodation of grain size reduction by three competing deformation mechanisms, i.e., dislocation, diffusion and dry-GBS creeps, involves a grain size reduction controlled by the sole dislocation creep at high temperatures (> 800 °C), whereas dislocation creep and dry-GBS creep, are the accommodating mechanisms at low temperatures (< 800 °C). Consequently, weakening is very limited if the grain size reduction occurs at temperatures higher than 800 °C, whereas a large weakening is expected in lower temperatures. This large weakening related to GBS creep would occur at depths lower than 60 km and therefore provides an explanation for ductile strain localisation in the uppermost continental mantle, thus providing an alternative to the brittle mantle.  相似文献   

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