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破裂带发展的扫描电镜实验研究及其对地震前兆的启示 总被引：17，自引：0，他引：17
在扫描电镜下对带割缝的大理岩试件进行了单轴压缩实验.在加载的全过程中,观察了试件表面裂纹的产生、扩展、平面分布以及断裂扩展前缘处的微裂纹在主断裂扩展前后的开、闭变化,并分析了它们与外载之间的关系.在显微照片上量测了主断裂的宽度随外载水平及测点所在部位的变化规律.在实验测定和结果分析的基础上,解释了脆性岩石材料在宏观裂纹扩展时的断裂能明显偏离线弹性断裂力学预测值的原因,提出了以标量作为岩石损伤力学中的损伤量的设想,探讨了实验结果对了解地震前兆（如大地形变和地下水位异常）可能起到的作用.将实验观察到的微破裂活动与1975年海城7.3级地震前地下水位异常做了对比分析,发现两者在时空分布方面有许多相似之处. 相似文献
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岩石受载内部微裂纹扩展及其震源机制反演有助于认识宏观裂纹扩展过程的非线性断裂力学行为.借助声发射监测手段,本文建立了仅涉及微裂纹张开/闭合和剪切滑移的位移不连续震源模型,通过各位置处传感器耦合质量标定及点源远场P波矩张量反演获得了含预制裂纹砂岩受载过程的震源机制解及时变响应特征,在全局坐标系下分析了微裂纹的三种断裂力学行为.结果表明:在位移不连续模型中,震源矩张量特征值与试样泊松比之间必须满足特定约束条件,该约束条件下的优化问题可采用拉格朗日乘子和Levenberg-Marquardt迭代法求解;受载砂岩裂纹扩展过程中,声发射震源以剪切滑移机制占优,微裂纹空间取向及运动方向与试样宏观主裂纹夹角平均值分别为40.9°和17.7°;对微裂纹体积分解表明岩体微观破裂机制以沿X方向I型张开为主,而沿Y方向的II型断裂滑移方向与试样全局变形方向相一致,由于试样内部晶粒分布非均质性造成了少量沿Z方向的III型平面外微裂纹滑移行为;受载砂岩裂纹扩展过程中微裂纹模式角与震源极性值变化趋势一致、利用震源震级评估的局部应力降值与实验观测结果相吻合,这两者均表明了位移不连续模型在震源机制定量反演中的适用性. 相似文献
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岩石破裂时电磁辐射的机理研究 总被引：21，自引：6，他引：21
本文提出了岩石破裂时的电磁辐射是裂纹尖端电荷随着裂纹加速扩展运动所产生的假说.应用断裂力学方法推导了岩石破裂时初始裂纹长度与裂纹扩展加速度的关系,并计算了其速度和加速度值.根据破裂岩石的电子发射理论,解释了裂纹尖端带电荷的现象.利用岩石在单轴压缩致裂过程中记录到的近场电磁辐射的实验结果,计算了裂纹扩展时裂纹尖端的电荷量和远场电磁辐射强度.通过对电磁辐射波谱分析的研究,得到岩石破裂时电磁辐射频率上限的估计值.最后对岩石破裂时出现的声光电磁现象在理论上作了统一的定性的解释. 相似文献
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断层三维扩展过程的实验研究 总被引：3，自引：0，他引：3
实验研究三维断层的形成和扩展对于理解实际断层作用过程具有重要意义．在双轴压缩条件下开展了断层三维扩展过程的实验研究,利用多通道数字化高密度应变观测和基于可见光图像分析的数字散斑相关测量技术对岩石样品应变场的详细结构进行了动态观测和分析,同时利用多通道声发射全波形三维定位系统对样品内部微破裂的发育过程进行了观测．实验结果表明,断层在三维空间的扩展模式与二维明显不同,表现出更复杂的空间展布形态和变形机制．断层的三维扩展过程可以划分为3个基本阶段：第一裂纹扩展阶段——翼裂纹扩展阶段、转换阶段——花瓣裂纹活动阶段和第二裂纹扩展阶段——贝壳断面形成阶段．不同阶段具有不同的主导裂纹扩展方式,并对应不同的变形场和微破裂分布．其中,花瓣裂纹活动阶段在三维断层的发育过程中至关紧要,它是从表面似二维扩展向三维扩展转换的关键,也是三维断层扩展区别于二维断层的核心所在。 相似文献
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本文根据地震的断层说观点在室温、围压600—1,200巴条件下研究了具切口的花岗闪长岩、辉长岩和大理岩试件的破裂发展过程。在连续增加的差应力作用下观测到:切口内部充填的软弱夹层首先发生剪切变形和破裂,接着在切口端部一侧扩展张性裂纹,然后在切口前缘方向扩展剪切裂纹,最后发生贯通试件的剪切和张裂-剪切主破坏。张裂纹扩展长度受到围压的强烈抑制。岩石的切口结构和岩性变化对破裂迹线的空间展布和主破坏机制有重要影响。讨论了实验结果在断层扩展型地震的形成过程及其在预报预测方面的意义 相似文献
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本文介绍了以激光全息干涉法观测单轴压缩下,大理岩岩样表面的变形位移场。全息干涉图可以反映出由于岩石内部微裂隙丛集激增所导致的变形局部化,实验采用板状大理岩试件,在中心处预制了不同角度的裂缝,实验在MTS伺服压机中加载直至宏观破坏,观测了裂隙的发展过程。实验表明:当裂缝角小于45时,先在裂缝尖端处的张应力集中部位出现新裂纹,它的起裂角(与原裂缝的交角)90,裂纹弯向压力方向并趋于稳定。当>45时,在上述张裂纹稳定后,在裂缝尖端附近再次发生张裂,其起裂角60,同样弯向压力方向后稳定。在这些前期张破裂稳定后,在张裂的相反方向,也即裂缝的共轭方向上,出现内部微裂隙的丛集,并随后发生宏观的剪破坏,我们认为此逆向剪切破坏与大理岩的多晶组构有关,与应变弱化过程中变形和应力的调整有关。 相似文献
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在单轴加压下进行了有预制裂纹的岩石板在裂纹扩展过程中声发射时b值的实验。发现b值的变化与岩石裂纹的扩展过程有密切关系,并且不同岩石介质的相互作用可影响b值的变化。通常裂纹扩展时,b值下降,但扩展受阻时,b值又有所回升,因此,有预制裂纹的岩石板在破裂过程中,b值呈起伏变化。 相似文献
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本文根据求得的无穷远边界上作用的外力主矢量为常量的共线双半无限长裂纹的平面问题的线性解答,分析了应力场的定性特征:张压应力区的边界和裂纹将全平面分成六个区域,其分布主要由外力主矢量的方向所决定。对线性解答及其稳定性问题的讨论,使我们可从理论上分析裂纹的扩展方式,求得较“库仑破裂准则”强的破裂条件(主要依赖于外应力主矢量的方向)並给出了破裂长度的近似表达式。根据地质力学的观点,在地震孕育的整个过程中,可假定外应力沿同一方向持续加强,计算表明弹性变形使得该方向相对于闭锁段发生偏转,从而使整个孕育过程按外应力主矢量所达到的特定方向分为两个阶段:第一阶段,裂纹无扩展,通过以时间为参数的附加应力场的计算,讨论了上述微小偏转所引起的应力场的变化;第二阶段,裂纹扩展,即闭锁段两端发生纯剪切位错,通过该双位错所引起附加应力场的计算分析了该阶段的应力特征,並探讨了地震序列与大震的关系。最后讨论了平面非共线双半无限长直裂纹问题,得到了前述类似的结论。 相似文献
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在隧道的施工和运营中,隧道衬砌不可避免会产生裂纹。裂纹和地震荷载的相互作用将加剧隧道的破坏,因此研究带裂纹隧道衬砌地震荷载作用下的破坏具有重要的意义。为了证明本文二维有限元数值模拟计算结果的正确性,首先用相互作用积分的方法计算动载作用下的静态裂纹,并与解析解进行比对,发现二者的吻合性很好。计算结果表明相互作用积分法可以用来精确地计算动载作用下带裂纹结构的动应力强度因子。用这种经过验证的方法来计算带裂纹重载铁路隧道衬砌的动应力强度因子和动承载力安全系数,可以看出在地震荷载作用下,I型裂纹的动应力强度因子在隧道结构的安全中起控制作用。当裂纹的长度大于某特定值时,隧道处于很危险的状态。 相似文献
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This paper discusses the applicability of the tension-softening model in the determination of the fracture toughness of rocks,
where the fracture toughness evaluated based on the tension-softening model is compared with the crack growth resistance deduced
from laboratory-scale hydraulic fracturing tests. It is generally accepted that the fracture process is dominated by the growth
of a fracture process zone for most types of rocks. In this study, the J-integral based technique is employed to determine the fracture toughness of Iidate granite on the basis of the tension-softening
model, where compact tension specimens of different dimensions were tested in order to examine the specimen size effect on
the measured fracture toughness. It was shown that the tension-softening relation deduced from the J-integral based technique allowed us to determine the specimen size independent fracture toughness Kc of Iidate granite. Laboratory-scale hydraulic fracturing tests were performed on cubic specimens (up to a 10 m sized specimen),
where cyclic pressurization was conducted using a rubber-made straddle packer to observe the extent of the hydraulically induced
crack. The experimental results of pressure and crack length were then used to construct the crack growth resistance curve
based on the stress intensity factor K. The crack growth resistance obtained from the hydraulic fracturing tests was observed to initially increase and then level
off, giving a constant K value for a long crack extension stage. The plateau K value in the crack growth resistance curve was found to be in reasonable agreement with the fracture toughness Kc deduced from the tension-softening relation. It was demonstrated that the tension-softening model provides a useful tool
to determine the appropriate fracture toughness of rocks, which may be applicable for the analysis of the process of large-scale
crack extension in rock masses. 相似文献
13.
G. A. Sobolev 《Pure and Applied Geophysics》1986,124(4-5):811-824
One of the simplest models of earthquakes and rockbursts was studied in laboratory conditions in which the fracture was initiated in a barrier between two preexisting faults. The treated models were built of concrete; during the construction of the models, the stress concentrators were inserted inside the models. This arrangement enabled the shear displacement to occur during uniaxial loading of the model. The tests were made on the series of models, the sizes of which were mutually varying more than one order. In the process of the barrier fracture propagation, the following were investigated: the time and space changes of local deformations as well as the acoustic emission, velocities and amplitudes of elastic waves, electrical conductivity and proper electro-induction. The process of barrier fracturing can be understood in three fundamental stages. In the course of the first stage, the density of small tensile cracks increases considerably, while the volume in which they exist is gradually enlarged. In the second stage, as the result, of these cracks coupling, longer shear cracks are created. During the coupling, due to the development of numerous regions of unstable deformation, the zones of nonequal rigidity arise in the treated medium, distributed within it in a mosaic-like pattern. In the third stage, the main fracture is prepared and formed with simultaneous unloading of the surrounding medium. The process of crack forming is gradually localized into a more narrow zone.The second and third stages of fracture forming are reflected in variations of all the above-mentioned physical parameters which are therefore identified as the precursors of the main fracture. By means of the series of precursors it is possible to find the reliable prediction of a barrier fracture. 相似文献
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Apparent fracture toughness in Mode I of microcracking materials such as rocks under confining pressure is analyzed based
on a cohesive crack model. In rocks, the apparent fracture toughness for crack propagation varies with the confining pressure.
This study provides analytical solutions for the apparent fracture toughness using a cohesive crack model, which is a model
for the fracture process zone. The problem analyzed in this study is a fluid-driven fracture of a two-dimensional crack with
a cohesive zone under confining pressure. The size of the cohesive zone is assumed to be negligibly small in comparison to
the crack length. The analyses are performed for two types of cohesive stress distribution, namely the constant cohesive stress
(Dugdale model) and the linearly decreasing cohesive stress. Furthermore, the problem for a more general cohesive stress distribution
is analyzed based on the fracture energy concept. The analytical solutions are confirmed by comparing them with the results
of numerical computations performed using the body force method. The analytical solution suggests a substantial increase in
the apparent fracture toughness due to increased confining pressures, even if the size of the fracture process zone is small. 相似文献
15.
T. Reuschlé 《Pure and Applied Geophysics》1998,152(4):641-665
—Fracture in a heterogeneous solid is simulated on a triangular network of bonds which figure the potential cracks of the medium. Heterogeneity is introduced by assuming a statistical strength distribution for the bonds. External stresses are applied to the network and the evolution of the bond population is analyzed when the stresses are increased. Bond-breaking is controlled by the crack-exten sion force which takes into account crack interactions by using an iterative procedure. Crack propaga tion leads to the coalescence of broken bonds crack clusters are formed. By using this kind of approach which combines fracture mechanics and network modelling, we are able to simulate the rupture of a rock specimen under various loading conditions without heavy computation. We discuss physical properties of the rupture process by examining the rupture stress and the geometric properties of the macroscopic fracture and their dependence on loading conditions and heterogeneity. Analysis of the geometric characteristics shows that the number of broken bonds can be fitted by a power law of the lattice size, the exponent depending on the loading conditions. Furthermore, an approximate computation of the mechanical response of the network demonstrates that the threshold secant modulus may be a more legitimate choice for a damage parameter in terms of system size independence. 相似文献
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按照压剪应力场中袭纹具有的特点,简化成三种力学模型——狭长缺口、顺序闭合裂纹及初始闭合裂纹。利用文中建议的局部分析法,对其端部应力场做的一般分析,导出了他们的普遍表达式。用光弹性实验及有限元计算对所得结果做的分析表明,它们是成立的。这些结果有助于了解构造地震震源的破裂机制及其应力场分布的某些特点。 相似文献
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L. N. Germanovich R. L. Salganik A. V. Dyskin K. K. Lee 《Pure and Applied Geophysics》1994,143(1-3):117-149
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In this paper, the micro-cracks in the brittle rocks are assumed to be penny shaped and evenly distributed; the damage and dilatancy of the brittle rocks is attributed to the growth and expansion of numerous micro-cracks under the local tensile stress. A single crack’s behaviour under the local tensile stress is generalized to all cracks based on the distributed damage mechanics. The relationship between the local tensile stress and the external loading is derived based on the Maxwell model. The damage factor corresponding to the external loading is represented using the p–alpha (p–α) model. A dilatancy equation that can build up a link between the external loading and the rock dilatancy is established. A test of dilatancy of a brittle rock under triaxial compression is conducted; the comparison between experimental results and our theoretical results shows good consistency. 相似文献