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1.
在冻融条件下岩石微裂隙中的水发生相变,体积膨胀,对微裂隙产生很大的冻胀力,当冻胀力超过岩石的抗拉强度时,微裂隙扩展。温度升高时,水又进入新的微裂隙,如此反复循环造成了岩石的损伤。据此,将岩石中的微裂隙等效为扁平状椭圆裂隙,基于断裂力学建立了单条微裂隙下裂隙扩展长度与冻胀力的关系,考虑岩石中微裂隙的分布,将岩石冻融条件下的应变分解为初始损伤应变、附加损伤应变和塑性应变,建立了弹塑性冻融损伤本构模型。最后,通过岩石冻融试验对该模型的合理性进行了验证,结果表明,该模型能够较好地模拟岩石在不同冻融次数下的应力-应变关系曲线。 相似文献
2.
Rock fracture under upper crustal conditions is driven not only by applied stresses, but also by time-dependent, chemically activated subcritical cracking processes. These subcritical processes are of great importance for the understanding of the mechanical behaviour of rocks over geological timescales. A macroscopic manifestation of time-dependency in the brittle field is the observation that rocks can deform and fail at constant applied stresses, a phenomenon known as brittle creep. Here, we review the available experimental evidence for brittle creep in crustal rocks, and the various models developed to explain the observations. Laboratory experiments have shown that brittle creep occurs in all major rock types, and that creep strain rates are extremely sensitive to the environmental conditions: differential stress, confining pressure, temperature and pore fluid composition. Even small changes in any of these parameters produce order of magnitude changes in creep strain rates (and times-to-failure). Three main classes of brittle creep model have been proposed to explain these observations: phenomenological, statistical, and micromechanical. Statistical and micromechanical models explain qualitatively how the increasing influence of microcrack interactions and/or the increasing accumulated damage produces the observed evolution of macroscopic deformation during brittle creep. However, no current model can predict quantitatively all of the observed features of brittle creep. Experimental data are limited by the timescale over which experiments are realistically feasible. Clearly, an extension of the range of available laboratory data to lower strain rates, and the development of new modelling approaches are needed to further improve our current understanding of time-dependent brittle deformation in rocks. 相似文献
3.
基于试验的花岗岩渐进破坏本构模型研究 总被引：7，自引：2，他引：5
对取自大渡河流域大岗山电站的花岗岩进行了系统的试验研究,得到了不同围压下的应力-应变曲线。根据岩样受力过程中内部微裂纹的活动状态,定义了4个特征应力,即闭合应力、起裂应力、破损应力、峰值应力,来反映花岗岩的渐进破坏过程,特征应力也反映了岩石内部的损伤程度。依据特征应力,将试验曲线分为4个阶段,并对每一阶段分别求取变形模量和泊松比。结果表明,变形模量不仅与围压有关,且与岩石的损伤程度有关,而泊松比只取决于岩石的损伤程度。特征应力可由体积应变曲线结合线性回归技术准确求取。在此基础上,提出了一个考虑花岗岩渐进破坏的本构模型。在该模型中,变形参数(弹性模量、泊松比)是应力状态的函数,强度参数（凝聚力、内摩擦角）是塑性变形的函数。将该模型嵌入大型有限元分析软件ABAQUS,对不同围压下的花岗岩室内压缩试验进行模拟,结果表明,模拟所得的应力-应变曲线与试验曲线的吻合程度较高,模型能反映花岗岩等脆性岩石的峰前非线性力学行为。 相似文献
4.
This article is devoted to numerical modeling of anisotropic damage and plasticity in saturated quasi‐brittle materials such as rocks and concrete. The damaged materials are represented by an isotropic poroelastic matrix containing a number of families of microcracks. Based on previous works, a discrete thermodynamic approach is proposed. Each family of microcracks exhibits frictional sliding along crack surfaces as well as crack propagation. The frictional sliding is described by a Coulomb–Mohr‐type plastic criterion by taking into account the effect of fluid pressure through a generalized effective stress concept. The damage evolution is entirely controlled by and coupled with the frictional sliding. The effective elastic properties as well as Biot's coefficients of cracked porous materials are determined as functions of induced damage. The inelastic deformation due to frictional sliding is also taken into account. The procedure for the identification of the model's parameters is presented. The proposed model is finally applied to study both mechanical and poromechanical responses of a typical porous brittle rock in drained and undrained compression tests as well as in interstitial pressure controlled tests. The main features of material behaviors are well reproduced by the model. Copyright © 2012 John Wiley & Sons, Ltd. 相似文献
5.
A new model for describing induced anisotropic damage in brittle rocks is proposed. Although phenomenological, the model is based on physical grounds of micromechanical analysis. Induced damage is represented by a second rank tensor, which is related to the density and orientation of microcracks. Damage evolution is related to the propagation condition of microcracks. The onset of microcrack coalescence leading to softening behaviour is also considered. The effective elastic compliance of the damaged material is obtained from a specific form of Gibbs potential. Irreversible damage‐related strains due to residual opening of microcracks after unloading are also captured. All the model's parameters could be determined from conventional triaxial compression tests. The proposed model is applied to a typical brittle rock. Comparison between test data and numerical simulations shows an overall good agreement. The proposed model is able to describe the main features related to induced microcracks in brittle geomaterials. Copyright © 2002 John Wiley & Sons, Ltd. 相似文献
6.
The stress-strain behaviour of rock material related to fracture under compression 总被引：12，自引：0，他引：12
Fracture is the main reason for the non-linear behaviour of hard rocks. The fracture mechanics of rock is studied in this article by analysis of the fracture process under compression. A constitutive model that describes the relationship between the macro deformation of rock and the micro fracture within rock is developed. The propagation of microcracks, the non-linearity of deformation, the loading-and-unloading hysteresis and the variation of the apparent Young's modulus and Poisson's ratio are studied using the developed model. The model simulations demonstrate that: (1) the fracture toughness, initial crack length, crack density, and Young's modulus are four crucially important parameters that affect the deformation behaviour of rock; (2) the elastic parameters (E and v) of the rock matrix should be measured in triaxial tests. If they are measured in uniaxial tests, the upper straight unloading portion of the stress-strain curve is suggested to be used for the purpose, unless the closure effect of open cracks will be included in the estimations. In addition (3), the slope of the reloading stress-strain curve is a measure of the damage in material. 相似文献
7.
CCSD主孔岩芯中发育有十分丰富的脆性微断层,孔深5158m以上,按其空间分布,可将其主体归纳为北北东向微断层系、北西向微断层系、北东向微断层组和近于东西向微断层组等四个微断层系（组）和SEE-NWW向水平挤压构造应力场、NE-SW向水平挤压构造应力场等二期区域构造应力场。SEE-NWW向水平挤压构造应力场贯穿于高压-超高压变质岩折返的全过程,表明在折返过程中,深层韧性变形阶段的构造应力场和浅层脆性变形阶段的构造应力场,具有高度的一致性。但流劈理和微断层的极点等值线图表明,韧性变形阶段的变形较脆性变形阶段的变形简单,深部发生的基本上是一种以逆冲型剪切应变为主导的变形,而浅部脆性变形域,除继承性的逆冲型剪切应变外,往往叠加有后期的构造伸展作用和走滑作用,因此具有更为复杂的应变图象。NE~SW向水平挤压构造应力场,在时间上晚于SEE~NWW向水平挤压构造应力场,它是导致先存的北北东向逆冲型流劈理发生自北东向南西方向滑动的主因。对比不同岩石类型的微断层和流劈理的极点等值线图,无论是极密类型,还是极密的分布,均不受岩石类型的影响,说明微断层和流劈理的形成与岩石类型（岩性）无关,而主要受构造因素制约,因此,运用微断层和流劈理（叶理）相结合的分析法,研究高压-超高压变质岩带折返阶段的构造应力场和动力学过程,有其他方法无可替代的效果。 相似文献
8.
岩石流动性和变形显微构造的发育直接受温度、压力、应变速率和流体相等制约 ,致使在不同地壳层次岩石的流动性表现出很大的差异。对上部地壳环境条件下天然和实验变形岩石的显微构造分析揭示出一系列具有不同特点以及由不同的成核、扩展和联合方式形成的破裂与微破裂型式的存在。讨论了在上部地壳环境中 ,温度与围压的变化对岩石破裂的影响 ,并阐述了高压破裂与低压破裂及其力学、流变学和显微构造特点 ,提出高压破裂对应于天然变形环境下出现的剪切 (挤压 )破裂 ,而碎裂岩带是典型的天然低压破裂 ,其低压环境的出现可以是浅部低围压或深部高流体压力所致。流体相的存在不仅可以引起石英 ,也可以引起方解石类碳酸盐岩矿物的水解弱化 ,并进而导致岩石流动机制的转变。岩石变形及流体等因素所致的岩石粒度变化 ,则从另一个方面影响着上部地壳岩石流动性的变化。从变形环境考虑 ,随着深度的加大 ,温度和压力升高 ,导致岩石由脆性向韧性转变 ;转变域内岩石的变形是一个复杂过程 ,是多种不同脆性和晶质塑性机制的综合。 相似文献
9.
10.
A boundary element model for stress/stability analysis of underground excavations in the vicinity of faults is presented. The boundary element formulation adopts the fictitious stress method for the simulation of excavation boundaries and the displacement discontinuity method for the representation of faults. The numerical model employs the Barton–Bandis non-linear joint model for the modelling of the fault behaviour and linear elastic behaviour for the rock. An incremental-iterative in situ stress relaxation algorithm is implemented for the non-linear analysis of the faults. Both deformation and peak strength models of Barton–Bandis are incorporated for modelling the mechanical behaviour of the fault. The non-linear deformation of fault considers the effects of coupling between shear and normal stresses and displacement, joint closure, joint separation, hardening followed by post-peak or residual behaviour. The peak strength model employs a mobilized non-linear shear strength envelope. The differences between linear and non-linear simulation of the fault models are discussed. A comparison of model predictions with the classical Mohr–Coulomb peak strength model with constant joint stiffness is presented. The numerical model is used for a case study of Canadian hard rock underground mine. The shear and normal displacements along the fault during four mining sequences with backfill simulation are presented and discussed. 相似文献
11.
A constitutive law for viscoelastic behaviour of rocks is derived from irreversible thermodynamics. To this model, two specific parameters are introduced; one is an internal state variable which is a variable concerning the microstructures such as defects in crystals or microcracks, and the other is a temperature reduced time obtained by normalizing the various temperature behaviours. A large number of internal state variables have the respective relaxation times and show the respective time evolutions, while a set of the time evolutions generates temporal power-law behaviour of rocks. The time evolutions of internal states are regarded as dynamics of elements of the generalized Maxwell model, and the stress–strain relation is represented by a response function following a temporal power-law in terms of linear system theory. This relation is inversely formulated to investigate the source field from output data. This model enables us to explain experimentally-based constitutive laws for transient and steady-state behaviour of rocks (e.g., lherzolite) following a temporal power-law and for attenuation behaviour of polycrystals (e.g., olivine) represented by a relation between the quality factor and frequency. Both laws show power-laws on deformation time or frequency depending on the fractal structure in polycrystals or rocks, and the experimental high-temperature behaviours can be extrapolated to long deformation time or high frequency behaviour. 相似文献
12.
Among three main stages of the process of earthquake nucleation long-, middle- and short-term the final stage is characterized by abrupt activation of the process of stress-strain state variation. The strain rates increase by orders of magnitude throughout the whole region of preparation, which increases the signal-to-noise ratio, and therefore the fracture, is easier to detect through monitoring geophysical parameters. The near-critical stresses existing in the Earth's crust and near the surface make it necessary to take into account the real rheology of the rocks, which, as is well known, is characterized by clearly pronounced plastic properties. The condition is favorable for developing creep processes in general and in its avalanche phase immediately before the fracture. The process is completely nonlinear but not chaotic. Based on the assumption that the attenuation of the stress-strain field is proportional to r− 3, a possible scenario of the final stage of earthquake nucleation process is proposed on the basis of the slip weakening mechanism in the source and the associated mosaic pattern of precursors on the Earth's surface. The formulas for estimating the ultimate distance of precursor detection and the duration of precursor events depending of normalized epicentral distance at the final stage of inelastic deformation preceding brittle failure of rocks are proposed. The data of electromagnetic precursors are interpreted in terms of a multiple fracture model. The results of in situ observations of electric field anomalies in the atmosphere are analyzed in relation to seismic activity. The possibility of constructing a physical model for the generation of a quasi-stable field and electromagnetic emission on the basis of the deformation process prior to an earthquake is discussed. Numerical estimates are obtained for polarization density and life time of an ensemble of electric dipoles generated in surface layers of the crust due to opening of microcracks and other dislocation mechanisms. The origin of quasi-constant electric field along a deformation region on a scale of the preparation zone is advantageous for the propagation of seismic anomalous atmospheric electric fields from the Earth's surface into the ionosphere. The field can be regarded as a physical agent of lithosphere–ionosphere connection. 相似文献
13.
引入损伤变量ω理论,分析水平状软硬相间岩层在竖向应力下的应力-应变关系：再引用弹性模量E和岩层厚度L两个变形参数建立软硬相间岩层底板变形参数方程,得出竖向应力随着底板深度的增加而减小的规律：运用数值模拟软件,建立煤层开采模型,模拟软硬相间岩层底板在采动作用下的变形过程。通过数值分析底板在采动作用下的应力-应变关系和位移特征,发现竖向应力作用下软岩受到的水平应力比硬岩大,竖向应变也比硬岩大,而竖向应力和水平应变变化不大,认为在采动影响下软硬相间岩层底板中的软岩具有吸收更多的应变能来保护软岩下硬岩的变形特点。 相似文献
14.
Time is one of the often-neglected factors in the assessment of the erratic failure of shale rock. Laboratory-creep experiments showed that constant stress induces time-dependent failure in brittle shale. However, the microscopic reason for time-dependent deformation in shale is still unknown. In the current study, triaxial creep and recovery experiments showed that the brittle shale specimens exhibit viscoelastic and viscoplastic creep deformation at constant stress state. In addition, the X-ray computed tomography scan of Marcellus shale showed that the shale specimens contained significant volume of preexisting microcracks. The statistical correlation among permanent strain during the triaxial experiment and stress-induced change in the three-dimensional geometry of microcracks showed that the microcracking is the microscopic reason for viscoplastic creep deformation in shale. In addition to the time and level of constant differential stress, factors such as orientation of bedding planes and specimen heterogeneity also influence the nature of creep deformation.
相似文献15.
Quartz microstructures developed during non-steady state plastic flow at rapidly decaying stress and strain rate 总被引：7，自引：0，他引：7
Synseismic loading to very high stresses (>0.5 GPa) and subsequent creep during stress relaxation in the uppermost plastosphere at temperatures of ca. 300–350 °C, near the lower tip of an inferred once seismically active crustal scale fault, was proposed based on peculiar microstructures identified in rocks exposed over >100 km2 in the Sesia Zone, European Western Alps. Here we discuss the conspicuous and highly heterogeneous microstructural record of quartz in disseminated small-scale shear zones. Sub-basal deformation lamellae and arrays of elongate subgrains on the TEM-scale indicate an early stage of glide-controlled deformation at high stresses. Distributed brittle failure is indicated by healed microcracks. Very fine-grained recrystallised aggregates with a pronounced crystallographic preferred orientation reflect intense plastic flow by dislocation creep. Locally, a fine-grained foam microstructure indicates a final stage of static grain growth at low differential stress. For the previously inferred peak stresses of about 0.5 GPa and given temperatures, initial strain rates on the order of 10−10 s−1 are predicted by available flow laws for dislocation creep of quartz. We emphasise the importance of short-term non-steady state deformation in the uppermost plastosphere underlying seismically active upper crust. The related heterogeneous record of quartz is governed by the local stress history at constant temperature. 相似文献
16.
In order to study the relationship between the deformation mechanism and permeability on brittle rock, the curves of stress–strain and permeability–strain of brittle rock were analyzed, the results indicated that the permeability of brittle rock increased rapidly at the critical failure point due to the microstructure changed seriously during the compaction, elastic deformation, and progressive failure process. When the rock bridges or asperities on the internal structural plane were ruptured partly or completely after the peak stress, a sudden decrease in rock strength occurred and the peak permeability could be the maximum. The strain at the critical point and turning point on the stress–strain curve corresponded to that at the rapid increase point and the peak point on the permeability–strain curve according to the renormalization theory and curves of stress–strain and permeability–strain. In addition, the ratios could be described by mathematical expressions. The conclusions could be proved reasonably by the experimental studies and examples of statistical analysis. 相似文献
17.
欢乐谷地区由新元古代泥砂质岩层夹铁镁质岩层组成。受达马拉期陆块碰撞事件的影响,发生区域中深地壳层次的强烈韧性变形。后碰撞期,在地壳增厚背景下,发生大规模伸展减薄和花岗岩浆作用,形成多种浅色花岗岩体即白岗岩。产铀白岗岩主要为D型及E型白岗岩,为S型壳源花岗岩。欢乐谷地区经历了四期五个阶段的构造演化,分别是:前达马拉期构造变形、达马拉碰撞造山期韧性变形(早阶段的挤压逆冲、晚阶段的走滑剪切韧性变形)、后达马拉期脆性变形和新生代整体抬升引起的脆性变形。广泛发育的白岗岩属于同构造期岩体。通过对变质岩和白岗岩的节理测量统计,基本确定了研究区的碰撞后区域应力场。最优势的主压应力方向介于N26°~35°方位间,其次为介于N110°~129°方位间和N345°~360°方位间的主压应力。目前保留在各类岩石中的密集节理构造,是碰撞造山后构造折返或岩浆上涌到达上地壳层次后才发生的,与铀矿富集关系密切。本研究初步探讨了达马拉期构造作用、韧性剪切、后期脆性断裂(基性岩墙侵位通道)与铀成矿作用的成因联系和制约作用。 相似文献
18.
David Amitrano 《Comptes Rendus Geoscience》2004,336(6):505-512
We propose a mechanical model for the behaviour of rocks based on progressive damage at the elementary scale and elastic interaction. It allows us to simulate several experimental observations: mechanical behaviour ranging from brittle to ductile, fractal structure of the damage, power-law distribution of the damage avalanches. These macroscopic properties are not incorporated at the elementary scale, but are the results of the interaction between elements. This emerging complexity permits us to consider the strain rock process as a complex system characterized by non-linear dynamics. To cite this article: D. Amitrano, C. R. Geoscience 336 (2004). 相似文献
19.
压缩作用下岩石内部细观裂纹扩展导致岩石产生损伤,其对岩石变形、强度等力学特性有着重要影响;然而,岩石内部裂纹扩展与剪切特性（黏聚力、内摩擦角及剪切应力）动态演化关系很少被研究。基于裂纹扩展机制推出的岩石应力-应变本构模型,并结合摩尔-库仑失效准则,推出了在岩石应力-应变关系峰值应力（对应岩石压缩强度）状态时,本构模型细观力学参数与岩石黏聚力、内摩擦角及剪切强度之间的状态关系。然后,引入岩石应力-应变本构关系塑性变形阶段服从摩尔-库仑屈服准则的力学流动规律,进而将已推出的应力-应变关系峰值状态点所满足的细观力学参数与黏聚力、内摩擦角关系,推广到岩石进入塑性变形后,岩石内部裂纹扩展（或应变）与黏聚力、内摩擦角及剪切应力动态演化的理论关系。随着裂纹扩展或应变增加,黏聚力、内摩擦角及剪切应力先增大,达到一个峰值点后减小,该结果与应力-应变本构曲线变化趋势相对应。通过试验结果验证了所提出理论结果的合理性。并讨论了初始裂纹之间摩擦系数对黏聚力、内摩擦角及剪切应力随裂纹扩展或应变演化规律的影响。 相似文献
20.
高地应力区地下岩体工程开挖常形成围岩拉-压应力状态,发生岩体张性破坏灾害。本文针对传统PFC平行黏结模型不能模拟脆性岩石高单轴压缩与拉伸强度比的问题,建立双抗拉强度参数的平行黏结强度准则,开展岩石拉-压数值模拟试验,得到了与物理试验接近的拉-压强度,实现了岩石高压拉强度比的模拟,并深入分析了破坏机制。研究结果表明随着围压的增加,破裂面倾角逐渐增大,由拉伸破裂转化为拉-剪破裂,发现了拉-压应力状态下破裂面处的雁行裂纹。根据细观颗粒位移场揭示了破裂面力学性质,随着围压的增加(破裂面倾角逐渐增大),破裂面张性逐渐减弱而剪性增强。可将拉-压应力状态下岩石损伤演化过程大致分为弹性变形阶段、稳定破裂发展阶段、不稳定破裂发展阶段和整体破裂阶段(峰后应力跌落及残余阶段)。围压较大时弹性变形和稳定破裂发展阶段相对较短,不稳定破裂发展阶段相对较长较剧烈,峰后残余阶段破裂面摩擦更强、应力波动较大。 相似文献