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1.
岩石构造对声发射统计特征的影响   总被引:25,自引:6,他引:19       下载免费PDF全文
利用一套最新型的全波形、宽动态声发射观测系统,对两种不同构造的花岗岩在三轴压缩变形实验中的声发射活动进行了对比研究。二者在声发射空间分布,声发射与体积扩容的对应关系,声发射频谱特征及频度能级统计参数等方面均有明显差异。这表明,岩石构造对声发射的基本统计特征有显著的控制作用。其原因在于岩石构造的差异造成变形方式和变形过程的不同  相似文献   

2.
对几种不同结构的岩石标本在变形过程中声发射b值和频谱随时间的变化特征进行了对比研究 ,其中包括完整花岗岩标本、含有天然愈合节理的花岗岩标本、含有拉张型和挤压型雁列式断层以及平直断层的标本等。研究表明 ,声发射b值和频谱的特征不仅会受标本结构的影响 ,而且在同一标本的不同变形阶段也可能表现出不同的特征 ,其机制与变形方式以破裂为主或以摩擦为主有关。当变形以破裂为主时 ,声发射b值和频谱在失稳前会出现明显的下降 ;当变形以摩擦为主时 ,声发射b值和频谱在失稳前变化相对较小 ,且上升或下降均可能出现。实验结果意味着b值和频谱特征作为失稳前兆 ,在不同的构造环境下可能会有不同的特征 ,而强震孕震区内不同断裂构造的存在会造成前兆时空分布的非均匀性  相似文献   

3.
本文利用两个频率通道同时接收花岗岩标本及石灰岩标本在不同单轴加压方式下的声发射信号,研究了从加压到破坏的整个形变过程中,不同频道接收到的声发射率的变化特征.发现在各种加压方式下,花岗岩和石灰岩在破坏前,由不同频率通道接收到的声发射率均急剧增长;而在破坏的瞬间,高频通道接收的声发射率增长快于较低频率通道的声发射率.这两点可用来预测岩石的破坏.声发射率随轴向应力的变化与加压方式有关.匀速加压,加压过程中保持一段时间恒压或降压均对应一定的声发射率状态.有可能通过追踪声发射情况,推测应力变化趋势.   相似文献   

4.
As the rock samples will produce abnormal signals of acoustic emission, microseismic and charge signals under external loading, the waveform comprehensive monitoring devices are used to synchronously monitor acoustic emission, microseismic and charge signals during the deformation and failure process of granite with fault zone under uniaxial compression. The results show that, the granite with fault zone has obvious synchronous precursory signals of acoustic emission, microseism and charge induction in the elastic deformation stage, and has high amplitude synchronous precursory signals in the instability destruction stage. The influence of fault zone on granite samples strength is remarkable, and the uniaxial compressive strength of samples with the fault zone is greatly reduced. With the angle of the fault zone decreasing, the uniaxial compressive strength of the specimens is reduced, the samples are more liable to instability and the energy of instability destruction is greater. With the fault zone angle of granite samples decreasing, the acoustic emission, microseismic and charge induction signals increase in the deformation and failure process of samples. The samples stress decreases when the acoustic emission, microseismic and charge induction precursory signals appear synchronously. The duration of acoustic emission, microseismic and charge induction precursory signals is increasing in the instability destruction stage. When the angle of the fault zone reaches 30°, the mutability of acoustic emission, microseismic and charge induction signal increases, the time to enter the dangerous stage is much earlier, and the acoustic emission events of large magnitude increase significantly, and the large angle faults of coal mine are more dangerous. The intensive and high amplitude synchronous precursory signals of acoustic emission, microseism and charge induction are produced before the instability destruction, and the signals duration is shorter. The intensive and strongest synchronous precursory signals of acoustic emission, microseism and charge induction are produced in the instability destruction, and the signals duration is longer. Acoustic emission monitoring data can better reflect the micro rupture of rock. And combined with the acoustic emission, microseismic and charge induction precursory signals, the precursory information of rock instability destruction can be obtained more accurately.  相似文献   

5.
The coda wave propagation path has received extensive attention as it is more sensitive to small changes in the medium than the direct wave. During the process of loading, the wave velocity, medium or source changes may cause the coda wave to change. The physical mechanism of change in the ultrasonic coda wave varies during different deformation stages. Meanwhile, there exist local damages in the rock sample during the deformation, and it will be accompanied by acoustic emission. Combining the ultrasonic coda wave and acoustic emission is beneficial to characterize the coda wave characteristics and damage degree of the sample at different deformation stages. In this paper, three kinds of rocks, including granodiorite, marble and sandstone with the sizes of 50mm×50mm×150mm, are used to carry out observations of ultrasonic coda wave and acoustic emission during the whole process of loading so as to study characteristics of the coda wave at different deformation stages. The major results are given below: 1)There is a good correspondence between the coda wave variation and the acoustic emission evolution process. When the acoustic emission frequency increases, the coda wave changes accordingly. In particular, the coda wave changes in the early stages of increased acoustic emission frequency, which indicates that the early damage information of rock can be obtained by analysis of the coda wave. 2)The physical mechanism of the coda wave change is different in different deformation stages. At the initial stage of loading, there are obvious scatterer changes in the coda wave change; then, in the linear elastic deformation stage, the wave velocity change is dominating; in the late-stage of loading, the scatterer change increases and coexists with the wave velocity change, the scatterer change effect is related with the rock micro-fracture degree, the rock will locally be damaged before rupturing, and the role of the scatterer will be enhanced. 3)With the increase of loading, the amplitude of increase of the wave velocity generally decreases gradually, which is basically consistent with the understanding obtained through the direct wave. The interference of acoustic emission can be eliminated because of the Kaiser effect when analyzing the coda wave. The consistency of the wave velocity change and stress loading and unloading is further verified. 4)The micro-fracture generated during rock deformation will change the physical mechanism of the coda wave change, and the scatterer effect will be significantly enhanced. At the same time, the acoustic emission waveform will cause interference to the ultrasonic coda wave. This means that attention needs to be paid when analyzing rock damage using only coda wave data. In short, the ultrasonic coda wave and acoustic emission can reflect the damage inside the rock, and the change mechanism of the coda wave in different deformation stages is different. The joint observation of the two can play a mutual verification role, which is conducive to improving the reliability of the observation results.  相似文献   

6.
岩石样品变形时的声发射   总被引:4,自引:0,他引:4       下载免费PDF全文
研究岩石样品变形过程中的声发射主要包括两个方面的内容:一是研究声发射事件的时空分布;二是研究声发射信号的振幅-频度分布。由于声发射活动性的研究与地震活动性的研究是十分相近的,所以实验室中对岩石样品声发射的研究有可能增进对地震活动性的认识。 本文总结了最近在声发射研究方面的一些结果,讨论了应力水平、加载时间和加载历史对岩石样品声发射活动性的影响,即讨论了在单调加载、静态疲劳加载和重复加载三种情况下的声发射特征。本文强调指出,即使是实验室内,利用声发射活动进行岩石样品的破坏预报方面仍然存在着一些困难。最后提出了解决这些困难的建议。  相似文献   

7.
巴卡.  M 《内陆地震》1996,10(1):79-85
通过对岩石样品进行变形及破坏试验,研究断裂形成过程中的声发射记录(AE),以找到能解释地震前兆现象的方法.另外,对试验过程中获得的大量数据及资料进行了数理统计处理.  相似文献   

8.
应力途径和破裂前兆   总被引:4,自引:1,他引:4       下载免费PDF全文
耿乃光  陈顒  姚孝新 《地震学报》1980,2(3):236-244
本文研究了在不同的应力途径下岩石破坏的条件和破裂的前兆.选定了三种应力途径进行研究:在一定应力状态下增加最大主应力σ1, 保持σ2, σ3不变, 使岩石破坏(A 型);减小最小主应力使岩石破坏(B 型);增加最小主应力岩石不破坏(C 型).通过实验得到了济南辉长岩和昌平花岗岩 A 型途径和 B 型途径破裂强度的比较.对三种途径岩石的体应变、声发射和波速Vp, 进行了对比研究.A 型途径的破裂前兆表现与许多作者的结果相符合.B 型途径岩石断裂前处于"过密"状态, 与此相联系的声发射增加和波速Vp下降出现得很晚.C 型途径岩石处于超膨胀状态, 出现了声发射增加和波速Vp下降而岩石并未破坏的现象.   相似文献   

9.
The mechanism and dynamics of the deformation and fracture of quartz, granite, and marble samples under the striker blow on their surface and electric discharge inside them are studied by the fractoluminescence (FL), electromagnetic (EME), and acoustic emission (AE) methods with 10-ns resolution. The impact excites a forced deformation wave with a velocity within 0.8 to 2 km/s depending on the mineral. The atomic bonds rupture and microcracks are formed at the nodes of the wave, which leads to the emergence of the FL flashes and disruption of the time dependences of EME. Based on the intensity of the flashes, the dimensions of microcracks are estimated to vary from 2 to 70 µm depending on the mineral. In turn, the emergence of microcracks initiates additional deformation waves.The discharge inside the studied samples excites a pressure shock wave which transforms into the tension wave after reflection from the surface. According to the analysis of FL spectra, this leads to the breakdown of the rocks into positively charged ions and electrons. The shock wave velocity in granites is measured at 4.8 km/s, which is close to the velocity of the longitudinal acoustic vibrations ~5 km/s. The microcracks in the rock have not enough time to form with this loading velocity. It is supposed that the shock wave stretches the deformed interatomic bonds at the dislocation nuclei in the crystal lattices of the minerals up to their breakdown into positively charged ions.  相似文献   

10.
Izvestiya, Physics of the Solid Earth - Laboratory experiments on monitoring the acoustic emission signals and time variations of volumetric activity of radon during uniaxial loading of a granite...  相似文献   

11.
岩石破裂过程中电磁辐射的实验研究   总被引:24,自引:5,他引:24       下载免费PDF全文
在单轴压力下对灰岩、花岗岩、石英岩三种样品的破裂过程与电磁辐射进行了实验室试验。结果表明,含有石英晶体的岩石,在破裂过程中产生的电磁信息,其振幅具有脉冲形态;随着应力水平的增高,电磁脉冲的频度增加,与声发射具有同步发展的趋势;不同结构的介质,主破裂前又呈现出平静和高潮两种不同类型。此外,含有石英晶体的岩石其主破裂及解体过程中,伴随最强的电磁脉冲,出现明显的闪光现象。文中对实验结果作了初步的讨论。  相似文献   

12.
岩石破裂中的光声效应   总被引:7,自引:1,他引:7       下载免费PDF全文
在实验室条件下研究了花岗岩样品受单轴压缩破裂过程中的光和声发射效应,所得可见光谱轮廓与空气分子的光谱相似,但具有能量高于紫光的成份。除在主破裂时有大的光脉冲和声发射外,在主破裂前也记录到弱的光脉冲,它们与大的声发射率有同步现象。  相似文献   

13.
Spheroidal weathering, one of the important rock weathering styles, has been attributed to chemical weathering by the water from joint surfaces, and mechanical aspects of the weathering have not been well addressed. We made an investigation on spheroidal weathering of Miocene granite porphyry with well‐developed columnar joints and found that this spheroidal weathering proceeds through chemical processes and accompanying mechanical processes. The investigation of the textures, physical properties, mineralogy, and chemistry of the porphyry revealed the presence of a brown band on the surface margins of corestones, representing the oxidation of pyrite and chlorite, and the precipitation of iron hydroxides, and the consequent generation of micro‐cracks within the band. During weathering, oxidation progresses inwards from joints that surround the rindlets, including both high‐angle columnar and low‐angle planar joints, and causes rounding of the unweathered interior portion of the rock. Microscopic observations of the brown band embedded with fluorescent resin show that pores are first filled with iron hydroxides, and that micro‐cracks then form parallel to the oxidation front in the outer portion of the brown band. Iron hydroxide precipitation increases the P‐wave velocity in the brown band, while micro‐crack formation decreases the tensile strength of the rock. Where the brown band has thickened to ~6 cm, the micro‐cracks are connected to one another to create continuous cracks, which separate the rindlets from the corestone. Micro‐crack formation parallel to the corestone surface may be attributed to compressive stresses generated by small amounts of volumetric expansion due to the precipitation of iron hydroxides in the brown band. Earth surface is under oxidizing environments so that precipitation of iron hydroxides commonly occurs; the spheroidal weathering in this paper is a typical example of the combination of chemical and mechanical processes under such environments. Copyright © 2016 John Wiley & Sons, Ltd.  相似文献   

14.
15.
震前地声与动物异常关系的研究   总被引:1,自引:0,他引:1       下载免费PDF全文
蒋锦昌  刘向群 《地震学报》1981,3(4):429-439
本文根据近十年来我国地声观测的某些结果, 分析了地声的时-空分布特点, 并估计了透入基岩面上和水面中的声压.同时与震前动物异常特点, 以及与人和某些动物的听觉和振动感受器的敏感阈值进行了比较.最后, 对唐山余震期间同时段内鱼和地声活动的观察结果, 进行了相关分析.其结果如下:1.地声和动物异常的时-空分布图式基本相似, 并可认为都是临震前兆.2.三级左右地震震中附近地区, 地声透入基岩面上和水面中的声压, 在150——250赫芝频段内, 分别为23——19分贝和90——86分贝.由此可见, 人耳是不可能感觉到的, 但是通常在地面上栖息的猫、狗、雉和穴居的鼠是可能觉察到的, 而骨鳔鱼类可能优先于这些陆生动物觉察到水中的地声信息.同时, 基岩面位移的垂直振幅约为10-7厘米.这虽比某些动物的振动感受器的阈振幅约低3个数量级.但可推测, 在强烈地震前的地面位移的垂直振幅可达到或超过微米量级.这就可能为这些动物的振动感受器觉察到.3.相距约20公里的鱼和地声活动观察点, 同期内的观察结果表明, 它们共同反映了同一地区内的唐山余震活动.同时, 鱼和地声活动的日频度序列之间具有一定的互相关性.   相似文献   

16.
This paper investigates the form of the nonwhiteness found in the reflection coefficients from a wide variety of rock sequences around the world. In all but one case densities are taken as constant due to the paucity of suitable density data. The reflection sequences are pseudo-white only above a corner frequency, below which their power spectrum falls away according to a power law fβ, where β is between 0.5 and 1.5. This spectrum can be adequately modelled in practice very simply with an ARMA (1, 1) process which acts on a white innovation sequence. The corollary of this is that before wavelet estimation methods are applied (all of which-except those based on synthetic seismograms—presuppose white reflection sequences) or deconvolution filters estimated, seismic traces should be filtered with the inverse of this process. Interestingly, the estimated ARMA processes group themselves into two clearly differentiated categories, having very different indices of predictability (or, strictly, indices of linear determinism). The two categories apparently correlate precisely with two kinds of sedimentation: one which consists largely of sequences of rocks with repeating properties, called “repetitive” in this paper but perhaps loosely describable as “cyclic”, and the other which is randomly bedded with no apparent pattern of components. The former has indices of predictability which are two to four times as great as those of the latter. Another, probably related, property is that β for the repetitive sequences tends to be greater than that for non-repetitive rock columns. The observed power spectra are shown to be consistent with a simple model for the logarithm of acoustic impedance consisting of a mixture of processes where the distribution of (time) scale parameters is reciprocal. Detailed effects of block-averaging and sampling the logs are shown to depend on the type of sequence under examination.  相似文献   

17.
The essential conditions for effective and ecologically safe exploitation of underground waste storage are maintenance, prevention, and monitoring of tightness of rock masses covering and surrounding the reservoir rock complex. This monitoring can be realized by a especially designed acoustic measurement system.The reservoir rock complexes - without leakage - are supposed to be in physical equilibrium; without changes of rock dynamic properties the acoustic emission vanishes. In contrast, as is shown, the results of the field tests carried out in coal mines proved that there was a correlation between the stresses and the acoustic emission ratio. The laboratory experiments also showed correlation between changes of permeability of coal samples and acoustic emission.the explanation of the observed results is based on the development of inelastic deformation of a rock skeleton. The plastic strains in the porous rock appear after overcoming the yield point. The yield point value can be extended by increase of shear stresses, effective stresses and interstitial pressure.In particular, there are three kinds of dynamic phases which may appear preceding the failure of leak tightness:
1. (1) breaking of the rock masses due to stress (Griffith criterion of stability may be expressed in terms of the acoustic emission parameters),
2. (2) the dilatant corrosion of pressure plasticity resulting from chemical, physical and thermal activities, and
3. (3) the destructive increase of pressure in rock pores.
This paper presents the statistical parameters describing the acoustic emission from the rock mass and the dynamic processes mentioned above are described in terms of seismoacoustic activity.  相似文献   

18.
不同应力途径三轴压缩下岩石的声发射   总被引:2,自引:2,他引:2       下载免费PDF全文
陈颙 《地震学报》1981,3(1):41-48
在不同加载方式的三轴实验中,观测了济南辉长岩和北京昌平花岗岩的声发射(围压达1.3千巴).当最大主应力增加使岩样破坏时(A型),平均声发射率逐渐增加,离破裂强度约几百巴时声发射急剧增多.而当岩石处于一定的高应力状态,通过减小围压使岩样破坏时(B型),声发射的急剧增加仅出现在离破裂差应力20-30巴的情况下,而且这种破裂过程声发射总数只有 A 型的1/3左右.在 B 型加载情况下,从应力场的球张量部分(流体静压力)来看,是一个卸载过程,而从偏张量部分来看,是一个加载过程.这种卸载过程的存在很可能是造成声发射不同特征的主要原因.   相似文献   

19.
Many granitic batholiths occur in the form of com-plexes, presented principally by a temporal-spacial association between two stages of intrusion, in the Nanling region. Compared with main intrusive gran-ites, late intrusive granites are characterized by fine- grained texture, Si- and Al-enriched composition, and small occurrence as stock or apophysis. On the basis of its rock chemistry (e.g., increasing aluminium saturation index) and geochemistry (e.g., Eu depletion, decreasing concentratio…  相似文献   

20.
The rapid release of strain energy is an important phenomenon leading to seismic events or rock failures during the excavation of deep rock.Through theoretical analysis of strain energy adjustment during blasting and mechanical excavation,and the interpretation of measured seismicity in the Jin-Ping Ⅱ Hydropower Station in China,this paper describes the characteristics of energy partition and induced seismicity corresponding to different energy release rates.The theoretical analysis indicates that part of the strain energy will be drastically released accompanied by violent crushing and fragmentation of rock under blast load,and this process will result in seismic events in addition to blasting vibration.The intensity of the seismicity induced by transient strain energy release highly depends on the unloading rate of in-situ stress.For mechanical excavation,the strain energy,which is mainly dissipated in the deformation of surrounding rock,releases smoothly,and almost no seismic events are produced in this gradual process.Field test reveals that the seismic energy transformed from the rock strain energy under high stress condition is roughly equal to that coming from explosive energy,and the two kinds of vibrations superimpose together to form the total blasting excavation-induced seismicity.In addition,the most intense seismicity is induced by the cut blasting delay; this delay contributes 50% of the total seismic energy released in a blast event.For mechanical excavation,the seismic energy of induced vibration(mainly the low intensity acoustic emission events or mechanical loading impacts),which accounts only for 1.5‰ of that caused by in-situ stress transient releasing,can be ignored in assessing the dynamic response of surrounding rock.  相似文献   

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