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1.
Shengli Ma Liqiang Liu Jin Ma Kaiying Wang Xiaoyan Hu Tianchang Liu Xiuquan Wu 《中国科学D辑(英文版)》2003,46(2):56-66
The nucleation process of stick-slip instability was analyzed based on the experimental measurements of strain and fault slip on homogeneous and non-homogeneous faults. The results show that the nucleation process of stick-slip on the homogeneous fault is of weak slip-weakening behavior under constant loading point velocity. The existence of a short “weak segment” on the fault makes slip-weakening phenomenon in nucleation process more obvious, while the existence of a long “weak segment” on the fault makes the nucleation process changed. The nucleation is characterized by accelerating slip in a local region and rapid increase of shear stress along the fault in this case, which is more coincident with the rate and state friction law. During the period when fault is locked, increasing of shear stress causes lateral elastic dilation near the fault, and the rebound of the dilation at the time of instability causes an instantaneous increase of normal stress in the fault plane, which is an important factor making fault be rapidly locked and its strength recovered. 相似文献
2.
本文利用GPS观测对丽江—小金河断裂带的现今断层运动和变形状态进行了分析和探讨.丽江—小金河断裂带两侧地块地壳变形差异显著,GPS速度剖面结果显示断裂带两侧存在地壳变形不连续现象;进一步以GPS速度场为约束,基于负位错模型反演的丽江—小金河断裂带的断层闭锁空间分布结果显示,以木里为界,北东段断层强闭锁从地表向深部延伸至15km左右,西南段断层闭锁程度较高的区域位于5～15km范围内,浅层表现为弱闭锁的状态;滑动亏损速率结果显示,两闭锁段的滑动亏损速率相差近4mm·a~(-1),说明丽江—小金河断裂带西南段的背景滑动速率明显高于北东段.基于数值模拟分析了西南段浅层蠕滑运动对周边断层的影响,结果表明西南段的浅层左旋滑动对北东段闭锁区和西南段深部强闭锁区均为正影响. 相似文献
3.
THE GEOLOGICAL AND ROCK MECHANICAL DISTINCTION EVIDENCE BETWEEN STICK-SLIP AND CREEP IN HOST ROCK SEGMENTS OF FAULT 
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下载免费PDF全文 ZHOU Yong-sheng 《地震地质》2019,41(5):1266-1272
Paleo-seismic and fault activity are hard to distinguish in host rock areas compared with soft sedimentary segments of fault. However, fault frictional experiments could obtain the conditions of stable and unstable slide, as well as the microstructures of fault gouge, which offer some identification marks between stick-slip and creep of fault.
We summarized geological and rock mechanical distinction evidence between stick-slip and creep in host rock segments of fault, and analyzed the physical mechanisms which controlled the behavior of stick-slip and creep. The chemical composition of fault gouge is most important to control stick-slip and creep. Gouge composed by weak minerals, such as clay mineral, has velocity weakening behavior, which causes stable slide of fault. Gouge with rock-forming minerals, such as calcite, quartz, feldspar, pyroxene, has stick-slip behavior under condition of focal depth. To the gouge with same chemical composition, the deformation mechanism controls the frictional slip. It is essential condition to stick slip for brittle fracture companied by dilatation, but creep is controlled by compaction and cataclasis as well as ductile shear with foliation and small fold. However, under fluid conditions, pressure solution which healed the fractures and caused strength recovery of fault, is the original reason of unstable slide, and also resulted in locking of fault with high pore pressure in core of fault zone. Contrast with that, rock-forming minerals altered to phyllosilicates in the gouges by fluid flow through degenerative reaction and hydrolysis reaction, which produced low friction fault and transformations to creep. The creep process progressively developed several wide shear zones including of R, Y, T, P shear plane that comprise gouge zones embedded into wide damage zones, which caused small earthquake distributed along wide fault zones with focal mechanism covered by normal fault, strike-slip fault and reverse fault. However, the stick-slip produced mirror-like slide surfaces with very narrow gouges along R shear plane and Y shear plane, which caused small earthquake distributed along narrow fault zones with single kind of focal mechanism. 相似文献
4.
利用二维有限元数值模型,结合断层滑移弱化摩擦准则对断层滑动规律以及应力扰动对其影响进行了研究．数值计算结果表明,在均匀应力分布情况下, 平面断层滑动显示出典型的特征地震规律,断层面上的应力扰动对断层滑动规律产生影响,压应力增加明显延迟地震的发生时间,并增加地震释放的能量．应力扰动发生在地震破裂临界区时的影响比在震前滑移区时的影响显著．当发生在地震滑移区时,若应力扰动足够大,则压应力增大会造成地震发生时部分动力断层被暂时锁住,使得地震释放的能量变小,但可增加后续地震的能量; 而压应力减小则可导致地震规律产生更加复杂的变化,会即时触发地震．如果应力扰动发生在一个地震周期的早期,则触发的地震较小,但可导致随后的地震提前发生; 如果应力扰动发生在一个地震周期的后期,则会触发大地震．当应力扰动位于震前滑移区或破裂临界区时,小的扰动也可能产生类似的效果．应力扰动产生越晚,这种影响也越明显．应力扰动发生在破裂临界区的影响最明显．应力扰动的影响一般主要集中在应力发生扰动后的1—2个地震周期内．后续地震基本恢复无应力扰动时的特征地震规律． 相似文献
5.
Based on dynamic rupture simulations on a planar fault in a homogeneous half-space, we investigated the nucleation processes using the time-weakening friction law. Both the characteristic time and the rupture speed in the nucleation asperity play an important role in determining rupture behaviors on a fault plane following the time-weakening friction law, with which rupture starts from a single point in the nucleation asperity and propagates at a given speed toward the boundary of the nucleation area. Rupture with a small characteristic time or a large rupture speed in the nucleation asperity propagates earlier from the hypocenter. Rupture following the slip-weakening friction law requires a smaller radius of nucleation patch to have similar rupture front contours of the time-weakening friction law. Even if the rupture velocity in the nucleation patch of the time-weakening friction law increases to infinity, the peak slip rate in the nucleation asperity is smaller than that of the slip-weakening law. The peak ground velocity distributions of ruptures following the two friction laws are also compared. 相似文献
6.
James R. Rice 《Pure and Applied Geophysics》1983,121(3):443-475
Constitutive relations for fault slip are described and adopted as a basis for analyzing slip motion and its instability in
the form of earthquakes on crustal faults. The constitutive relations discussed include simple rate-independent slip-weakening
models, in which shear strength degrades with ongoing slip to a residual frictional strength, and also more realistic but
as yet less extensively applied slip-rate and surface-state-dependent relations. For the latter the state of the surface is
characterized by one or more variables that evolve with ongoing slip, seeking values consistent with the current slip rate.
Models of crustal faults range from simple, single-degree-of-freedom spring-slider systems to more complex continuous systems
that incorporate nonuniform slip and locked patches on faults of depth-dependent constitutive properties within elastic lithospheric
plates that may be coupled to a viscoelastic asthenosphere.
Most progress for the rate and state-dependent constitutive relations is at present limited to single-degree-of-freedom systems.
Results for stable and unstable slip with the various constitutive models are summarized. Instability conditions are compared
for spatially uniform versus nonuniform slip, including the elastic — brittle crack limit of the nonuniform mode. Inferences
of constitutive and fracture parameters are discussed, based on earthquake data for large ruptures that begin with slip at
depth, concentrating stress on locked regions within a brittle upper crust. Results of nonlinear stability theory, including
regimes of complex sustained stress and slip rate oscillations, are outlined for rate and state-dependent constitutive relations,
and the manner in which these allow phenomena like time-dependent failure, restrengthening in nearly stationary contact, and
weakening in rapidly accelerated slip, is discussed. 相似文献
7.
Finite Element Analysis of Fault Bend Influence on Stick-Slip Instability along an Intra-Plate Fault
— Earthquakes have been recognized as resulting from stick-slip frictional instabilities along the faults between deformable rocks. A three-dimensional finite-element code for modeling the nonlinear frictional contact behaviors between deformable bodies with the node-to-point contact element strategy has been developed and applied here to investigate the fault geometry influence on the nucleation and development process of the stick-slip instability along an intra-plate fault through a typical fault bend model, which has a pre-cut fault that is artificially bent by an angle of 5.6° at the fault center. The numerical results demonstrate that the geometry of the fault significantly affects nucleation, termination and restart of the stick-slip instability along the intra-plate fault, and all these instability phenomena can be well simulated using the current finite-element algorithm. 相似文献
8.
In order to analyze 3-dimensional movement and deformation characteristics and seismic risk of the Xianshuihe fault zone, we inverted for dynamic fault locking and slip deficit rate of the fault using the GPS horizontal velocity field of 1999-2007 and 2013-2017 in Sichuan-Yunnan region, and calculated annual vertical change rate to analyze the vertical deformation characteristics of the fault using the cross-fault leveling data during 1980-2017 locating on the Xianshuihe fault. The GPS inversion results indicate that in 1999-2007, the southeastern segment of the fault is tightly locked, the middle segment is less locked, and the northwestern segment is basically in creeping state. In 2013-2017, the southeastern segment of the fault is obviously weekly locked, in which only a patch between Daofu-Bamei is locked, and the northwestern segment is still mostly in creeping state, in which only a patch at southeastern Luhuo is slightly locked from surface to 10km depth. The cross-fault leveling data show that annual vertical change rate of the Zhuwo, Gelou, Xuxu and Goupu sites on the northwestern segment is larger, which means vertical movement is relatively active, and annual vertical change rate of the Longdengba, Laoqianning, and Zheduotang sites on the southeastern segment is small, which means the fault is locked, and the vertical movement changes little before and after the Wenchuan earthquake. Combining with the 3-dimensional movement and deformation, seismic activity and Coulomb stress on the Xianshuihe Fault, we consider the seismic risk of the southeastern segment is larger, and the Wenchuan earthquake reduced the far-field sinistral movement and the fault slip deficit rate, which may reduce the stress and strain accumulation rate and relieve the seismic risk of the southeastern segment. 相似文献
9.
Interaction of a Dynamic Rupture on a Fault Plane with Short Frictionless Fault Branches 总被引：1，自引：0，他引：1
Ronald L. Biegel Charles G. Sammis Ares J. Rosakis 《Pure and Applied Geophysics》2007,164(10):1881-1904
Spontaneous bilateral mode II shear ruptures were nucleated on faults in photoelastic Homalite plates loaded in uniaxial compression.
Rupture velocities were measured and the interaction between the rupture front and short fault branches was observed using
high-speed digital photography. Fault branches were formed by machining slits of varying lengths that intersected the fault
plane over a range of angles. These branches were frictionless because they did not close under static loading prior to shear
rupture nucleation. Three types of behavior were observed. First, the velocity of both rupture fronts was unaffected when
the fault branches were oriented 45° to the main slip surface and the length of the branches were less than or equal to ~0.75
R0* (where R0* is the slip-weakening distance in the limit of low rupture speed and an infinitely long slip-pulse). Second, rupture propagation
stopped at the branch on the compressive side of the rupture tip but was unaffected by the branch on the tensile side when
the branches were ~1.5 R0* in length and remained oriented 45° to the principle slip surface. Third, branches on the tensile side of the rupture tip
nucleated tensile ``wing tip' extensions when the branches were oriented at 70° to the interface. Third, when the branches
were oriented at 70° to the interface, branches on the tensile side of the rupture tip nucleated tensile ``wing-crack' extensions.
We explain these observations using a model in which the initial uniaxial load produces stress concentrations at the tips
of the branches, which perturb the initial stress field on the rupture plane. These stress perturbations affect both the resolved
shear stress driving the rupture and the fault-normal stress that controls the fault strength, and together they explain the
observed changes in rupture speed. 相似文献
10.
使用双剪粘滑模型模拟自发地震和诱发地震的区域加载过程,利用应变观测系统多点连续观测发震断层附近的局部应变变化。在应力与应变空间上描述了地震过程的区域应力路径和局部应变路径。结果表明,局部应变路径与应力宏观路径的形态差异较大,但两者的转换阶段对应,存在一定映射关系。断层局部变形路径的走向标明了断层所处在的变形阶段。自发地震的应变路径可以划分为3个部分:应变积累阶段、剪应变的线性偏离阶段和失稳滑动阶段。诱发地震的应变路径包括4个阶段:正斜率的应变积累阶段、负斜率的稳态滑动阶段、亚稳态应变僵持阶段、扰动失稳滑动阶段。自发地震与诱发地震有各自的路径模式,可以从应变路径上判别断层稳定性与可能的地震类型。 相似文献
11.
实验研究断层黏滑过程的变形演化,尤其是失稳黏滑瞬间的断层位移演化特征,对于了解地震从孕育到发生的全过程具有重要意义.本文基于数字散斑相关方法(digital speckle correlation method, DSCM),用三套图像采集系统(两套低速和一套高速图像采集系统)搭建了断层黏滑过程的多观测区域、多时间尺度的变形场测量系统,并用此系统对一种花岗岩双剪滑动模型的黏滑过程进行了实验研究.对间黏滑期和黏滑期断层位移演化特征进行深入分析的结果表明:间黏滑期断层位移演化体现出空间上的非均匀性和时间上的"趋同化"特征,断层滑动趋同化也许是断层错动匀阻化的一种宏观表现形式;断层黏滑动态过程持续时间非常短(本文300 mm断层黏滑过程持续时间约在1 ms量级),黏滑失稳前会出现预滑,预滑出现到黏滑失稳发生所经历的时间与黏滑失稳过程所用时间相差一个量级;断层的一次黏滑由若干个滑动速度不同的、小的失稳滑动组成,黏滑失稳过程中断层的滑动速度呈现出波动性,整个滑动过程中断层经历了多个高速滑动和低速滑动的交错. 相似文献
12.
本文研究了有限长度含有单一粗糙面的垂直走滑断层的滑动弱化不稳定性.我们假定断层强度在其深度方向是均匀的,而在走滑方向是不均匀的,即存在一个高强度段.并假定断层上的粗糙段及断层上的其它部分具有相同类型的本构律,只是峰值应力不同.断层周围的地壳材料用上、下表面应力自由的弹性平板来模拟.我们用有限元方法研究了理论位移场、应力场和应变场随远场位移的演变情况.此时,断层位移和摩擦应力并不是预先给定的,而是在求解过程中同时确定的.根据计算结果,我们比较了理论位移场及断层上摩擦应力分布在稳定和不稳定滑动情况时的差别.并与内部含有低强度段的走滑断层的场合做了比较. 相似文献
13.
用双剪法对济南辉长岩和点苍山大理岩进行了摩擦滑动实验.实验中的应力变化方式有两种.A 型实验:先使断层面上的正应力增加到一定值,然后保持正应力不变,并增加剪应力使断层发生粘滑;B 型实验:先使断层面上的正应力增加到一定的值,保持正应力不变,并增加剪应力到断层发生粘滑前的某一应力状态,再保持剪应力不变,减小正应力直到粘滑发生.实验表明,B 型实验中岩石的摩擦强度高于 A 型实验.A 型实验中粘滑发生前有声发射率增加的前兆,B 型实验中粘滑发生前看不到声发射率的明显增加.由实验得到一个启示,即闭锁断层的开锁可能采取两种形式:一种是冲开闭锁,即以剪应力的增加使断层发生错动;另一种是解开闭锁,即以正应力的减小使断层发生错动.断层的粘滑采取哪种形式,由断层带的应力变化途径决定. 相似文献
14.
Nicholas W. Hayman Lucie Ducloué Kate L. Foco Karen E. Daniels 《Pure and Applied Geophysics》2011,168(12):2239-2257
It is a long-standing question whether granular fault material such as gouge plays a major role in controlling fault dynamics
such as seismicity and slip-periodicity. In both natural and experimental faults, granular materials resist shear and accommodate
strain via interparticle friction, fracture toughness, fluid pressure, dilation, and interparticle rearrangements. Here, we
isolate the effects of particle rearrangements on granular deformation through laboratory experiments. Within a sheared photoelastic
granular aggregate at constant volume, we simultaneously visualize both particle-scale kinematics and interparticle forces,
the latter taking the form of force-chains. We observe stick-slip deformation and associated force drops during an overall
strengthening of the shear zone. This strengthening regime provides insight into granular rheology and conditions of stick-slip
periodicity, and may be qualitatively analogous to slip that accompanies longer term interseismic strengthening of natural
faults. Of particular note is the observation that increasing the packing density increases the stiffness of the granular
aggregate and decreases the damping (increases time-scales) during slip events. At relatively loose packing density, the slip
displacements during the events follow an approximately power-law distribution, as opposed to an exponential distribution
at higher packing density. The system exhibits switching between quasi-periodic and aperiodic slip behavior at all packing
densities. Higher packing densities favor quasi-periodic behavior, with a longer time interval between aperiodic events than
between quasi-periodic events. This difference in the time-scale of aperiodic stick-slip deformation is reflected in both
the kinematics of interparticle slip and the force-chain dynamics: all major force-chain reorganizations are associated with
aperiodic events. Our experiments conceptually link observations of natural fault dynamics with current models for granular
stick-slip dynamics. We find that the stick-slip dynamics are consistent with a driven harmonic oscillator model with damping
provided by an effective viscosity, and that shear-transformation-zone, jamming, and crackling noise theories provide insight
into the effective stiffness and patterns of shear localization during deformation. 相似文献
15.
With co-seismic surface rupture slip displacements provided by the field observation for the 2001 MS8.1 West Kunlun Mountain Pass earthquake, this paper estimates the rupture speed on the main faulting segment with a long straight fault trace on the surface based on a simple slip-weakening rupture model, in which the frictional overshoot or undershoot are involved in consideration of energy partition during the earthquake faulting. In contrast to the study of Bouchon and Vallée, in which the rupture propagation along the main fault could exceed the local shear-wave speed, perhaps reach the P-wave speed on a certain section of fault, our results show that, under a slip-weakening assumption combined with a frictional undershoot (partial stress drop model), average rupture speed should be equal to or less than the Rayleigh wave speed with a high seismic radiation efficiency, which is consistent with the result derived by waveform inversion and the result estimated from source stress field. Associated with the surface rupture mechanism, such as partial stress drop (frictional undershoot) associated with the apparent stress, an alternative rupture mechanism based on the slip-weakening model has also been discussed. 相似文献
16.
Weakening of a prestressed sawcut in Westerly granite under laboratory condition is accomplished by injecting pressurized fluid into the sawcut. After injection a sequence of stick-slips is observed while the deviatoric stress decreases successively with each stick-slip. On the basis of the experimental observation we develop a model of fault instability due to inhomogeneous and progressive weakening of the fault. According to this model, the fault surface is divided into the slipped and the locked regions, depending on whether or not the local state of stress satisfies the friction criterion. The average shear stress in the slipped region decreases with time and, in order to maintain a quasi-static equilibrium, shear stress in the remaining locked region on the fault surface increases. This situation may last until a critical state of stress on the fault is met, at which a sudden instability (stick0slip) may occur. We suggest that this mechanism of stress transfer may be a viable mechanism of induced seismicity and aftershocks, in addition to the well-known mechanism of a local increase of pore pressure. By comparing the experimental data with model predictions we show that the critical condition for slip instability is when the average shear stress over the locked region becomes equal to the value given by the friction criterion. Thus the friction criterion established for slip on fractures on which the state of stress is macroscopically uniform may also be applicable to fractures on which the stress state is macroscopically heterogeneous. 相似文献
17.
EXPERIMENTAL STUDY OF TEMPERATURE EVOLUTION AND IDENTIFICATION OF INSTABILITY POSITION OF PLANAR STRIKE-SLIP FAULT DURING PROCESS OF STICK-SLIP 下载免费PDF全文
下载免费PDF全文 Stick-slip of fault in laboratory accompanies change of temperature. Temperature change is not only concerned with sliding friction, but also with the stress state of the sample. In this article, we use infra-red thermal imaging system as wide-range observation means to study the temperature variation of different stages during the deformation of sample. The rock sample for the experiment is made of granodiorite from Fangshan County with a size of 300mm×300mm×50mm. It is cut obliquely at an angle of 45°, forming a planar fault. Two-direction servo-control system was used to apply load on the sample. The load in both directions was forced to 5MPa and maintained constant (5MPa) in the X direction, then the load in the Y direction was applied by a displacement rate of 0.5μm/s, 0.1μm/s and 0.05μm/s successively. The left and below lateral of the sample were fixed, and the right and top lateral of the sample were slidable when loaded. The experiment results show not only the temperature change from increase to decrease caused by conversion of stress accumulation to relaxation before and after the peak stress, but also opposite variation of temperature increase on fault and temperature decrease in rock during instability stage. Most important of all, we have found the temperature precursor identifying the position of instability through the temperature variation with time along the fault. It shows that rate of temperature increase of instability position keeps relative high value since the stage of strongly off-linear stage, and accelerates in stage of meta-instability. After separating the effect of friction and stress, we found that temperature increase occurs in the rock near the fault instead of on the fault, which means the mechanism of temperature increase is stress accumulation. Temperature of fault at the instability position does not increase, which means the position is locked. We speculate that the position of locked area on fault with high stress accumulation near the fault may be the future instability position. It is of significance of studying temperature variation during stick-slip to the monitoring of earthquake precursors. Heat caused by friction of earthquake needs long time to transfer to the surface and could not be detected as a precursor. While the stress of surface rock near the fault would change as the stress of interior rock changes, which could cause detectable temperature variations. The research purpose of this article is to find special change positions before instability. As the temperature variations are caused by stress and slip of fault, the results are also meaningful to analysis of stress and displacement data related to earthquake precursors. 相似文献
18.
利用2001年昆仑山口西MS8.1地震现场观测所提供的地表破裂同震位移数据,使用简单滑移弱化破裂模型,估算了发震主断层上的破裂传播速度. 该模型中考虑了断层破裂时动摩擦过程中应力上调和下调机制对地震波辐射能量分配的影响. 对比Bouchon和Valleacute;e有关昆仑山口西地震主断层破裂传播速度超过剪切波速度,甚至达到P波速度的结果, 采用动摩擦应力下调时的滑移弱化模型 (分数应力降模型),结果表明,伴随较高的地震波辐射效率,主断层的平均破裂传播速度等于或小于瑞利波速度,这与许力生和陈运泰的体波反演结果,以及陈学忠震源应力场估算的结果是一致的. 最后,联系到由地表破裂现象所反映出的断层力学特征,如与视应力相关的分数应力降 (动摩擦应力下调), 基于滑移弱化模型, 讨论了可能的震源破裂机制. 相似文献
19.
20.
Frictional heat generation and seismic radiation in a foam rubber model of earthquakes 总被引：1，自引：0，他引：1
Results from a study of stick-slip particle motion at the interface between two stressed foam rubber blocks indicate that normal vibrations and interface separation are an important part of the stick-slip process in foam rubber. The dimension of the dynamic slip pulse is small compared to the dimension of the model (approximately 10 cm vs. 200 cm) consistent with the abrupt-locking slip pulse model ofBrune (1970, 1976), andHeaton (1990). A comparison of frictional heat generation between stable-sliding and stick-slip foam rubber models indicates a linear relation between the temperature increase on the fault surface (for a given distance of slip) and the driving shear force for the stable-sliding model, while for the stick-slip model there is essentially no variation in frictional heat generation with an increase in shear stress. We performed experiments to investigate the ratio of normal motion to shear motion at different levels of normal stress in the stick-slip foam rubber model. Preliminary result indicate that the normal component of the particle motion increases more rapidly with increasing normal stress than the shear component. The phenomenon of interface separation and normal vibrations may thus explain some of the most frustrating problems in earthquake mechanics, e.g., the heat flow paradox, the long-term weakness of major active faults, and anomalousP-wave radiation. 相似文献