Mechanical analysis of en echelon structure and its significance of controlling earthquakes

ＭｅｃｈａｎｉｃａｌａｎａｌｙｓｉｓｏｆｅｎｅｃｈｅｌｏｎｓｔｒｕｃｔｕｒｅａｎｄｉｔｓｓｉｇｎｉｆｉｃａｎｃｅｏｆｃｏｎｔｒｏｌｌｉｎｇｅａｒｔｈｑｕａｋｅｓＸｉｎ－ＳｈｅｎｇＸＩＥ（谢新生）ａｎｄＸｉａｏ－ＰｉｎｇＲＵＡＮ（阮小平）（Ｉｎｓｔｉｔ...     

Mechanical analysis of en echelon structure and its significance of controlling earthquakes

The paper deals with the mechanical origin and rules ofen echelon folds and their secondary fractures by means of elastic stability theory and nonlinear fracture criterion. Obtains the quantitative relations amongen echelon angles ofen echelon folds, ratios of boundary stresses anden echelon pitches of shear zone under an action of general boundary forces (tension shear, pure shear or compression shear). As an applied example, the paper researches the displacement field, stress field, distortion energy distribution, state of secondary fractures and energy released by fracturing ofen echelon fold structure developed at the east foot of Taihang Mountain. The results of research show that maximum principal (compressive) stresses, maximum shear stresses, high value area of distortion energy are in the nuclear parts ofen echelon folds. In these parts compressive fractures were easily developed in approximately parallel with fold axis. So it is verified that the secondary fracture ofen echelon folds is a mechanism controlling a strong earthquake.     

Mechanical analysis ofen echelon structure and its significance of controlling earthquakes

The paper deals with the mechanical origin and rules ofen echelon folds and their secondary fractures by means of elastic stability theory and nonlinear fracture criterion. Obtains the quantitative relations amongen echelon angles ofen echelon folds, ratios of boundary stresses anden echelon pitches of shear zone under an action of general boundary forces (tension shear, pure shear or compression shear). As an applied example, the paper researches the displacement field, stress field, distortion energy distribution, state of secondary fractures and energy released by fracturing ofen echelon fold structure developed at the east foot of Taihang Mountain. The results of research show that maximum principal (compressive) stresses, maximum shear stresses, high value area of distortion energy are in the nuclear parts ofen echelon folds. In these parts compressive fractures were easily developed in approximately parallel with fold axis. So it is verified that the secondary fracture ofen echelon folds is a mechanism controlling a strong earthquake.     

The state of stress in the Earth's crust as based on measurements in mines and on geophysical data

Measurements of stress carried out in mines suggest that much of the Earth's crust is in a state of horizontal compression. The average of the two principal horizontal stresses usually exceeds the hydrostatic (geostatic) pressure and fits N. Hast's empirical relationship of increasing excess compressive stress with depth. High compressive stresses are usually aligned perpendicular to the trends of young, folded mountain ranges and to axes of positive and negative gravity anomalies.     

欧亚地震带现代构造应力场及其分区特征

利用美国哈佛大学矩心矩张量目录中的2818个地震的震源机制解资料,分析了欧亚地震带及其5个分区现代构造应力场的基本特征,给出了5个分区的震源机制主压应力方向分布图。结果表明:①欧亚地震带以逆断型和走滑型断层活动为主;②地中海地震区以走滑断层活动为主,主压应力方向为SSW向;③伊朗—阿富汗—巴基斯坦地震区以逆断型断层活动为主,主压应力优势方向为NNE—NS向;④喜马拉雅地震以逆断型为主,主压应力优势方向为NS和NE向;⑤川—滇—缅地震区以走滑断层活动为主,主应力场方向为NNE向;⑥印度尼西亚地震区以逆断型断层活动为主,主压应力优势方向为NE—SSW向。各分区的主压应力方向明显受其所在区域板块运动的影响,由此推测板块运动可能是产生欧亚地震带构造应力的主要力源。     

郯庐断裂带鲁苏皖段构造应力场及分段特征研究

利用Snoke方法求解和收集得到的77次中小地震的震源机制解资料, 采用Gephart应力张量反演方法, 获得了郯庐断裂带鲁苏皖段构造应力场, 最大主压应力方位角为80°, 最小主压应力方位角为172°, 最大、 中等和最小主压应力倾角分别为15°、 65°和19°, 反映了研究区处于近EW向水平作用和近NS向的水平拉张作用环境下。 根据地震活动、 地质构造及震源机制解差异, 我们将郯庐断裂带鲁苏皖段分5个区段开展研究, 结果显示: 5个分区应力场存在局部差异, 最大主压应力方位角处于63°～88°之间, 从北往南总体方向成顺时针偏转的趋势。 跨郯庐断裂带两侧的应力场研究结果显示, 从西到东最大主压应力方向有一个逆时针偏转的趋势, 西侧最大主压应力方向更接近EW向, 东侧更接近NE向, 郯庐断裂带内处于两侧的过渡地段。     

Effect of Sliding Rate on the Activity of Acoustic Emission During Stable Sliding

--The mechanical and statistical characteristics of acoustic emission (AE) events during stable sliding are investigated through a laboratory experiment using a granite specimen with a pre-cut fault. Numerous AE events are found to be generated on the pre-cut fault, indicating that microscopically unstable fracture occurs during macroscopically stable sliding. The composite focal mechanism solution of AE events is determined from the first motion directions of P-waves. The determined mechanism is consistent with the double-couple one expected for the slip on the pre-cut fault. The source radii of large AE events are estimated to be about 10 mm from the widths of the first P-wave pulses. These indicate that the AE events are generated by shear fracture whose faulting area is a part of the pre-cut fault plane. The occurrence of AE events as a stochastic process approximately obeys the Poisson process, if the effect of mutually dependent events consti tuting clusters is corrected. The observed amplitude-frequency relation of AE events approximately follows a power law for a limited amplitude range. As the macroscopic sliding rate increases, the number of AE events per unit sliding distance decreases. This rate dependence of the AE activity is qualitatively consistent with the observation that the real area of contact between sliding surfaces decreases with an increase in the sliding rate as reported in the literature.     

Experimental study of ultralong wave band for electro－magnetic signals and acoustic emission during rock fracture

Ｅｘｐｅｒｉｍｅｎｔａｌ　ｓｔｕｄｙ　ｏｆ　ｕｌｔｒａｌｏｎｇ　ｗａｖｅ　ｂａｎｄ　ｆｏｒ　ｅｌｅｃｔｒｏ－ｍａｇｎｅｔｉｃ　ｓｉｇｎａｌｓ　ａｎｄ　ａｃｏｕｓｔｉｃ　ｅｍｉｓｓｉｏｎ　ｄｕｒｉｎｇ　ｒｏｃｋ　ｆｒａｃｔｕｒｅ（曹惠馨）（钱书清）（吕...     

DC-induced acoustic emission in saturated sand models of sedimentary rock

The results of laboratory experimental studies of the DC-induced acoustic emission (AE) in saturated sand models of sedimentary rock are presented. It is shown that direct current acting on a geological medium generates acoustic vibrations in it. The experimental methodology is based on recording acoustic pulses generated by the rock model (sample) when the electric field is applied. The amplitude-frequency parameters of the AE signals depend on petrophysical properties of the solid phase, on the salinity of porous medium, and the electric field (current intensity and voltage). The above research is the first step towards the full identification of the characteristics of the AE signals generated by rocks in a DC electric field.     

Preliminary stress measurements in central California using the hydraulic fracturing technique

Use of the hydraulic fracturing technique for determiningin situ stress is reviewed, and stress measurements in wells near the towns of Livermore, San Ardo, and Menlo Park, California are described in detail. In the Livermore well, four measurements at depths between 110 and 155 m indicate that the least principal compressive stress is horizontal and increases from 1.62 to 2.66 MPa. The apparent direction of maximum compression is N 70° E (±40°). At the San Ardo site the least principal stress is that due to the overburden weight. At depths of 240.2 and 270.7 m the minimum and maximum horizontal stresses are estimated to be 11.4 and 22.5 MPa, and 12.0 (±1.1) and 15.8 (±3.3) MPa, respectively. From an impression of the fracture at 240.2 m, the direction of maximum compression appears to be about N 15° E. The rock in the Menlo Park well is too highly fractured to yield a reliable measurement of the horizontal stresses. The data indicate, however, that the least principal stress is vertical (due to the overburden weight) to a depth of 250 m.     

The effect of seismic uplift on the shell stresses of liquid‐storage tanks

Previous theoretical studies have shown that tank uplift, that is, separation of the tank base from the foundation, generally reduces the base shear and the base moment. However, there is a paucity of experimental investigations concerning the effect of uplift on the tank wall stresses, which is the principal parameter that controls the seismic design of liquid‐storage tanks. This paper reports a series of shake table experiments on a polyvinyl chloride model tank containing water. A comparison of the seismic behaviour of the tank with and without anchorage is described. Stochastically generated ground motions, based on a Japanese design spectrum, and three tank aspect ratios (liquid‐height/radius) are considered. Measurements were made of the stresses at the outer shell of the tank, the tank wall acceleration and the horizontal displacement at the top of the tank. While the top displacement and the tank shell acceleration increased when uplift was allowed, axial compressive stresses decreased by between 35% and 64% with tank uplift. The effect of uplift on the hoop stresses was variable depending on the aspect ratio. A comparison of experimental values with a numerical model is provided. Copyright © 2015 John Wiley & Sons, Ltd.     

Numerical modeling of the distribution of horizontal stresses in a moving continental plate

The distribution and time evolution of overlithostatic horizontal stresses in the vertical cross-sections of the model of a solid continent are studied in terms of a 2D numerical model. The continent is moving self-consistently with time-varying mantle flows. Over a period of 50 Ma, the continent, which had been initially located at a distance of about 1500 km from the downward mantle flow (subduction zone), first overlays the region of the marginal sea, then thrusts over the zone of subduction, thus making it inclined and deforming it. It is found that the horizontal tensile stresses observed at the initial stages are succeeded by compressive stresses, especially at the leading edge (up to 40 MPa). This is caused by the change of the dragging action of the subduction zone into the retarding action during the continent crossing over this zone. The dependence of the calculated stresses on the Rayleigh number and on the thickness of the model of the continent is estimated. It is obtained also that the distribution of horizontal stresses along the strike of the continent is rather distinctly indicative of the locations of upward and downward flows in the subcontinental mantle. With the considered values of the model parameters, the tensile stresses in the near-to central regions of the continent may be twice to thrice the tensile stresses at its margins. Hence, in the simplest case of a homogeneous continent, its division will occur in the zone directly above the upward subcontinental flow. Detachment from the continent of the fragments of its edge adjacent to the marginal sea implies that the thickness of the continental plate in that part and/or its strength is considerably lower than in the center of the continent.     

主应力轴持续旋转条件下饱和松砂的振动孔隙水压力特性

利用新研制的“土工静力-动力液压三轴-扭剪多功能剪切仪”,针对福建标准松砂,在三向非均等固结条件下,进行了能够模拟海洋波浪荷载作用下主应力轴连续旋转的循环耦合剪切试验。通过试验着重探讨了初始主应力方向、振动过程中主应力方向连续变化对不排水条件下砂土的振动孔隙水压力增长特性的影响。实验研究表明:在振动过程中主应力轴连续旋转的条件下,初始主应力方向对砂土的动孔压比与振次比之间关系具有显著的影响,随着初始大主应力与竖向之间夹角的增大,动孔压比的增长速度明显加快,具有较好的规律性;归一化孔压比与广义剪应变之间的关系基本上与初始主应力方向角和振动剪应力幅值无关。     

1992兰德斯地震震源处应力量值的研究

给出了根据地震前后应力轴偏转、地震应力降和地震前后相对主应力大小,计算震源处应力量值的方法.并将该方法运用于兰德斯地震的霍姆斯特德谷断层段,获得了该子断层10 km深度处震前最大、中间和最小主应力的量值分别为271,266 MPa和259 MPa;震前断层面上的正应力和剪切应力分别为265MPa和6.2 MPa;震后断...     

渤海湾盆地黄骅坳陷应力场的三维数值模拟分析

采用有限元方法模拟了渤海湾盆地黄骅坳陷的现今应力场特征.模型的构建主要基于黄骅坳陷精细三维地震数据体,包括了七个主要层序底面及近真实的断层产状.根据模拟结果,对比已知油气藏的分布位置和断裂的展布方向,定量分析了黄骅坳陷第一主应力、第三主应力、应力强度以及主应力方向的分布特征,并探讨了影响黄骅坳陷构造特征的主要因素.据此,得出以下认识:1)通过改变模型的边界条件发现,在右旋剪切作用下模型中压性应力场低值区的分布特征及主应力方向分别与黄骅坳陷中已知油藏的分布及断裂展布方向具有较好的对应关系.2)黄骅坳陷内构造样式及其构造应力场方向自北向南存在一定的差异,而造成这种差异的原因与地形的变化、沧东断层空间形态的变化、断层组合样式的变化以及滑脱面的变化密切相关.     

Syntheses of the regional stress fields of the Japanese islands

The principal stresses in northern Honshu and in central-southwest Japan are synthesized on the basis of the ridge push, slab pull and across-arc variation of differential forces due to crust/plate structural variation. Assuming a more compressive north–south horizontal stress in central Japan-northern Honshu than that of southwest Japan, the calculated principal stress profiles explain the observed stress fields in these areas: namely, a strike–slip fault type for southwest-central Japan and a reverse fault type for northern Honshu, both having east–west σ_Hmax. Kyushu is characterized by the gradient of horizontal stresses both in the east–west and north–south directions, which cannot be explained by simple plate interactions or by crust/plate structural variation. Combined with other lines of evidence for existence of mantle upwelling in the East China Sea west of Kyushu, it is proposed that the stress gradient is produced by the viscous drag exerted by the flow spread laterally from the upwelling plume. The eastward movement of Kyushu and southwest Japan relative to Eurasia revealed by the recent Global Positioning System measurements conducted by the Geographical Survey Institute of Japan would be partly explained by this basal drag.     

Granite deformation and behavior of acoustic emission sequence under the temperature and pressure condition at different crust depths

IntroductionFocal depths of shallow strong intraplate earthquakes are mostly distributed in the highstrength range of lithosphere controlled by the rheology property of granite and diorite (Brace,Kohlstedt, 1980; Sibson, 1982; Meissner, Strehlau, 1982; CHEN, Molnap 1983). This is obviouslyrelated to the change of rock deformation characteriStics at different crust depths. So, for earthquake stUdy, both of the rock failure types (fractUre or rock flow) and its mechanical instabilityforms (…     

Hypocenter distribution and focal mechanism of AE events during two stress stage creep in Yugawara andesite

More than a thousand acoustic-emission (AE) hypocenters were determined in a cylindrical andesite specimen under two-stage uniaxial creep at stresses of 204 and 214 MPa. Strains were monitored for 6 peripheral points at the middle part of the cylindrical specimen's wall. The strain data indicate gradual increase of nonuniform deformation during steady creep and strong intensification of the nonuniformity during acceleration creep and, therefore, biased stress distribution within the specimen. The correlation between dilatant strain and AE hypocenters was investigated for whether or not tensile cracks emit AE. The region with high AE activity shows only a small dilatant strain. This negative correlation between AE and the dilatant region may eliminate tensile cracks as possible AE sources. A composite focal-mechanism solution of local AE events, covering a wide solid angle of the focal hemisphere, indicates that shear fractures emit AE waves. The direction of the compressional axis in this solution shows a significant deviation from that inferred from the applied external force, suggesting that the local stress field is governed by preexisting weak zones that are, presumably, produced by tensile cracks within the specimen. AE hypocenters tended to form clusters during steady creep under the constant compressional stress. During acceleration creep caused by a small step increase of the external stress, the preceding clusters disappeared while a new cluster appeared in an incipient fault plane. This suggests that changes in seismicity pattern such as migrations or quiescences of swarm—important clues for earthquake predictions—may be caused by an instantaneous change in the tectonic-stress levels.     

确定岩石中先存应力状态的声发射法

对经过三向预加压的石灰岩试件所进行的试验研究表明,其声发射活动的特点与单向受力时的情况完全不同。此时,在一个试件的一次加载过程中会出现两次Kaiser效应,分别对应于载荷达到预加压时所施加的轴压与围压值之时。利用回归分析的方法来处理试验数据,可以使声发射活动对应力的响应关系用三条回归直线来近似。这三条直线的两个交点所对应的应力值,可以确定出预加压时岩石试件承受的应力状态     

Ultrasonic wave propagation in dry and brine-saturated sandstones as a function of effective stress: laboratory measurements and modelling1

Compressional and shear-wave velocities have been measured and a novel approach using digital processing employed to study wave attenuation for brine- and gas- saturated sandstones, over a range of effective stresses from 5 to 60 MPa. Also measured were the complex conductivity in the brine-saturated state and permeability in the gas-saturated state over the same range of stresses as for the velocity measurements. Broadband ultrasonic pulses of P- and orthogonally polarized S-waves in the frequency range 0.3–0.8 MHz are transmitted through the specimen to be characterized for comparison with a reference (aluminium) having low attenuation. The attenuation is calculated in terms of the quality factor Q from the Fourier spectral ratios, using the frequency spectral ratios technique. The corrections necessary for the effects of diffraction due to the finite size of the ultrasonic transducers have been carried out for the case of measurements under lower confining stress. To interpret the laboratory measured velocity and attenuation data under the physical conditions of this study and to estimate the effects of pore structure, numerical modelling of velocities and attenuation as functions of the confining stress have been performed, based on the MIT model. Theoretical models based on several hypothesized attenuation mechanisms are considered in relation to laboratory data of the effects of confining pressure, fluid saturation and pore structure on attenuation. Numerical calculations using these models with the experimental data indicate that friction on thin cracks and grain boundaries is the dominant attenuation mechanism for dry and brine-saturated sandstones at low effective stresses for the frequencies tested. However, for brine-saturated sandstones at moderately high effective stresses, fluid flow could play a more important role in ultrasonic S-wave attenuation, depending on the pore structure of the sample.