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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.
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
3.
An appreciation of the physical mechanisms which cause observed seismicity complexity is fundamental to the understanding
of the temporal behaviour of faults and single slip events. Numerical simulation of fault slip can provide insights into fault
processes by allowing exploration of parameter spaces which influence microscopic and macroscopic physics of processes which
may lead towards an answer to those questions. Particle-based models such as the Lattice Solid Model have been used previously
for the simulation of stick-slip dynamics of faults, although mainly in two dimensions. Recent increases in the power of computers
and the ability to use the power of parallel computer systems have made it possible to extend particle-based fault simulations
to three dimensions. In this paper a particle-based numerical model of a rough planar fault embedded between two elastic blocks
in three dimensions is presented. A very simple friction law without any rate dependency and no spatial heterogeneity in the
intrinsic coefficient of friction is used in the model. To simulate earthquake dynamics the model is sheared in a direction
parallel to the fault plane with a constant velocity at the driving edges. Spontaneous slip occurs on the fault when the shear
stress is large enough to overcome the frictional forces on the fault. Slip events with a wide range of event sizes are observed.
Investigation of the temporal evolution and spatial distribution of slip during each event shows a high degree of variability
between the events. In some of the larger events highly complex slip patterns are observed. 相似文献
4.
The relationship between the slip activity and occurrence of historical earthquakes along the Median Tectonic Line (MTL), together with that of the fault systems extending eastward has been examined. The MTL is divided into three segments, each containing diagnostic active faults. No historical earthquakes have been recorded along the central segment, although the segment has faster Quaternary slip rates compared with the other segments that have generated historical earthquakes. This discrepancy between earthquake generation and slip rate can be explained by a microplate model of southwest Japan. The microplate model also provides spatial and temporal coupling of slip on adjacent fault systems. In the context of this model, slip on adjacent faults reduces the normal stress on the MTL. Historical data and paleoseismic evidence indicate that slip on this segment occurs without significant strong ground motion. We interpret this as indicating anomalously slow seismic slip or aseismic slip. Slip on the central segment of the MTL creates transpressional regions at the eastern and western segments where historical earthquakes were recorded. Alternatively, the earthquakes at the eastern and western segments were triggered and concentrated shear stress at the edge of the segments resulted in postseismic slip along the central segment. The sequence of historical events suggests that the MTL characteristically does not produce great earthquakes. The microplate model also provides a tectonic framework for coupling of events among the MTL, the adjacent fault systems and the Nankai trough. 相似文献
5.
郯庐断裂带中段全新世活断层的特征滑动行为与特征地震 总被引：16，自引：0，他引：16
郯庐断裂带中段全新世活断层由３个独立的破裂段组成。从各破裂段的运动性质、位移分布看，断层的运动属特征地震型滑动。地震活动以强震活动为主，强震具有周期性原地重复发生的特点，且其强度基本相同；中强地震缺失或很少发生；ｂ值在高震级范围内具低ｂ值的非线性关系。这些特点正是特征地震的典型表现．根据郯庐断裂带中段活断层全新世以来的活动特点看，未来该区仍然以特征地震方式活动．按郯庐带的强震复发间隔和各段的最新一次活动时代推算，未来一段时期内新沂－宿迁段复发大震的可能性较大，安丘段次之，莒县－郯城段复发大震的可能性则很小。 相似文献
6.
利用1999—2007期和2009—2013期中国大陆GPS速度场数据,采用DEFNODE负位错反演程序估算了川滇菱形块体东边界——鲜水河—安宁河—则木河—小江断裂带在汶川地震前后的断层闭锁程度和滑动亏损空间分布动态变化特征,讨论了汶川地震对该断裂系统的影响范围和程度,并结合b值空间分布和地震破裂时-空结果分析了断裂系统的强震危险段.结果表明,汶川地震前鲜水河断裂最南端为完全闭锁(闭锁深度25km),中南段地表以下10~15km深度为强闭锁状态,中北段基本处于蠕滑状态;安宁河断裂最南端闭锁很弱,其余位置闭锁深度为10~15km;则木河断裂除最南端闭锁较弱以外,其余位置基本为完全闭锁;小江断裂在巧家以南、东川以南、宜良附近、华宁以北等四处位置闭锁较弱,其余位置为强闭锁.10年尺度的GPS速度场反演所得断层闭锁程度所指示的强震危险段,主要为鲜水河断裂道孚—八美段、安宁河断裂中段、则木河断裂中北段、小江断裂北段东川附近、小江断裂南段华宁—建水段,该结果与地质尺度的断层地震空区和30年尺度的b值空间分布所指示的危险段落具有一致性.汶川地震后断裂带远、近场速度分布和块体运动状态发生变化,这种区域地壳运动调整使得负位错模型反演得到的断裂带闭锁情况发生一定变化.汶川地震前后川滇菱形块体东边界平行断层滑动亏损速率均为左旋走滑亏损,且在安宁河断裂北端、则木河断裂中北段滑动亏损速率最大;除鲜水河断裂中南段与最南端和小江断裂东川附近以外,其余断裂震后滑动亏损速率均有所增加.垂直断层滑动亏损速率既有拉张亏损也有挤压亏损,且鲜水河断裂最南端由震前挤压转变为震后拉张,其余断裂除了安宁河断裂和小江断裂中段与最北端存在挤压滑动亏损速率外均为拉张速率. 相似文献
7.
由宽频带辐射能量目录和地震矩目录给出的视应力及其地震学意义 总被引：24，自引：2，他引：24
对NEIC宽频带地震辐射能量目录和哈佛矩心矩张量（CMT）目录的比较，给出了关于视应力的一些可能是有意义的结果，尽管目前的结果误差仍很大，可靠性也是有限的，但这种比较所提供的线索却颇值得注意，视应力的计算给出关于地震断层面上非线性动摩擦函数的线索，能量／地震矩之比随地震大小的变化表明，在BK模型框架下，对于走滑型地城,依赖于滑动速度的摩擦似乎占主要地位，而对于非走滑型地震，依赖于位移的摩擦似乎占主要地位，主震和余震的能量／地震矩之比的比较表明，对于走滑型地震，余震的视应力平均地说来低于主震的视应力，而对于非直滑型地震，余震的视应力即有高于主震的也有低于主震的，这对于障碍体和凹凸模式的讨论及模型中地震破裂停止条件的设置可能具有一定的参考意义。 相似文献
8.
A numerical method of viscoelastic finite element coupled with spring-block model is developed to study temporal processes from the slow tectonic motion of large-scale crust to the rapid failure of small-scale faults. Our modeling demonstrates that the motion of crustal blocks is driven by forces from tectonic plate boundaries, and the deformation is distributed on faults for the stress accumulating. The coupling model generates earthquake sequences that display a magnitude-frequency scaling consistent with Gutenberg-Richter law. The frictional heterogeneities affect earthquakes occurrence and stresses distribution of crustal blocks. Rupture of earthquakes starts at the nucleation node, and propagates bilaterally along faults with the stress triggering, release and redistribution. The failure of faults releases part of crustal stresses, the stress state of crustal blocks near fault is affected by the rupture of local segments on the fault, and the stress state of crustal blocks far away from the fault is controlled by the seismic activity of the whole fault. 相似文献
9.
A numerical method of viscoelastic finite element coupled with spring-block model is developed to study temporal processes from the slow tectonic motion of large-scale crust to the rapid failure of small-scale faults. Our modeling demonstrates that the motion of crustal blocks is driven by forces from tectonic plate boundaries, and the deformation is distributed on faults for the stress accumulating. The coupling model generates earthquake sequences that display a magnitude-frequency scaling consistent with Gutenberg-Richter law. The frictional heterogeneities affeci earthquakes occurrence and stresses distribution of crustal blocks. Rupture of earthquakes starts at the nucleation node, and propagates bilaterally along faults with the stress triggering, release and redistribution. The failure of faults releases part of crustal stresses, the stress state of crustal blocks near fault is affected by the rupture of local segments on the fault, and the stress state of crustal blocks far away from the fault is controlled by the seismic activity of the whole fault. 相似文献
10.
采用速度和状态摩擦本构控制的一维弹簧滑块模型研究断裂分段间相互作用对运动特征的影响,为研究东昆仑活动断裂带库赛湖段和西大滩段2个断裂分段之间的相互影响,采用由弹簧相连的2个滑块模拟断裂分段,通过弹簧滑块系统的动力学分析,将断裂运动性质的描述归结为一组微分方程,数值求解该微分方程组,最终得到断裂运动性质的参数,从而达到确定断裂未来强震复发周期的目的。通过位错模型计算、借鉴前人研究成果以及古地震资料确定模型相关参数。研究断裂分段在不同相互作用下的强震复发周期,模拟表明断裂间不同相互作用对地震复发周期和地震时断裂错动位移的大小没有规律性的影响;只是对地震发生时断裂错动的速度有明显的影响,作用强时,地震发生时断裂错动速度大;反之,地震发生时断裂错动速度小。 相似文献
11.
速率和状态相依赖的摩擦定律是本文采用的重要定律。结合Chester-Higgs摩擦模型和McKenzie-Brune摩擦生热模型,在一维弹簧-滑块-断层近似模型下,利用四阶变步长的Dormand-Prince算法,研究探讨了断层摩擦生热对断层演化的影响。结果表明:与忽略温度影响的情形相比,摩擦生热造成的温度上升可导致断层滑移时刻的略微提前,并伴随着摩擦系数和状态变量的下降,同时也使得断层的滑移量和应力降略有减小,而滑移速率有所增大;另外,在考虑温度影响时,有效正应力和临界滑移距离也会影响断层的演化过程,断层上的有效正应力越大,断层失稳时刻越提前,温度上升越明显;断层的临界滑移距离越大,断层失稳时刻则越迟,温度上升越显著,但当临界滑移距离超过5 cm时,具有不同临界滑移距离的断层,失稳时的温度则基本保持一致。 相似文献
12.
目前有两种最常用的岩石摩擦本构关系,其主要区别在于是否与静接触时间有关。对这两种本构关系的基本性质进行了对比研究,得出如下结论：（１）在匀速滑动的稳态附近,两种本构关系趋向一致;（２）在正应力恒定条件下,两种本构关系的主要差异在于克服摩擦力所需能量的大小。与静接触时间相关的本构关系在粘滑中需消耗较大的能量来克服摩擦阻力,在粘滑的减速段,这种本构关系可达到的最低速率比另一种本构关系低１０个数量级;（３）在正应力变化条件下,与静接触时间相关的本构关系基本继承了正应力恒定条件下的行为特征,而另一种本构关系在剪应力－速度相平面上却出现了一个长尾巴,使最低滑动速率降到比正应力恒定时的值低１０多个数量级 相似文献
13.
Assessing current faulting behaviors and seismic risk of the Anninghe-Zemuhe fault zone from seismicity parameters 总被引：6，自引：0，他引：6
Introduction Strong and large earthquakes are prepared and generated on specific segments of active fault zones, especially on the asperity parts of the zones (Aki, 1984; Wiemer, Wyss, 1997; Wyss, et al, 2000). Therefore, both the faulting-behavior identification and the rupture segmentation mainly based on the method of active tectonics are always important aspects in active fault research (DING, et al, 1993). The purposes of the two aspects of research focus on determining fault units tha… 相似文献
14.
Numerical Simulation of Earthquake Nucleation Process and Seismic Precursors on Faults 总被引：5，自引：0，他引：5
He Changrong 《中国地震研究》2000,14(3):199-212
To understand precursory phenomena before seismic fault sliP,this work focuses onearthquake nucleation process on a fault plane through numerical simulation.Rate and statedependent friction law with variable normal stress is employed in the analysis.The resultsshow that in the late stage of nucleation process:(1)The maximum slip velocity ismonotonically accelerating;(2)The slipping hot spot(where the slip rate is maximum)migrates spontaneously from a certain instant,and such migration is spatially continuous;(3)When the maximum velocity reaches a detectable order of magnitude(at least one orderof magnitude greater than the loading rate),the remaining time is 20 hours or longer,andthe temporal variation of slip velocity beyond this point may be used as a precursoryindicator;(4)The average slip velocity is related to the remaining time by a log-log linearrelation,which means that a similar relation between rate of microseismicity and remainingtime may also exist;(5)when normal stress variation is taken int 相似文献
15.
Can a simple multi-block-spring model with total symmetry make interesting predictions for fault behaviour? Our model consists of a symmetric, slowly driven, two degree-of-freedom block-spring system with static/dynamic friction. The simple friction law and slow driving rate allow the state of this fourth order system to be described between slip events by a single variable, the difference in the stretch of the driving springs. This stretch difference measures the locked-in stress and is closely related to fault stress inhomogeneity. In general,smoothing is not observed. A spatially homogeneous stress state is found to almost always be unstable, in that the system tends toward an inhomogeneous state after many slip events. The system evolves either to a cycle that alternates between two types of earthquakes, or to a cycle with repeating but identical asymmetric earthquakes. One type of alternating earthquake solution is structurally unstable, which implies a great sensitivity to model perturbations. For this simple model, spatial asymmetry necessarily occurs, despite the symmetry in the model, thus suggesting that spatial structure in seismicity patterns may be a consequence of earthquake dynamics, not just fault heterogeneity. 相似文献
16.
Dynamic faulting under rate-dependent friction 总被引：2，自引：0，他引：2
We discuss the effects of rate-dependent friction on the propagation of seismic rupture on active faults. Several physicists using Burridge and Knopoff's box and spring model of faulting have proposed that fault complexity may arise from the spontaneous development of a self-similar stress distribution on the fault plane. If this model proves to be correct, it has important consequences for the origin of the complexity of seismic sources. In order to test these ideas on a more realistic earthquake model, we developed a new boundary integral equation method for studying rupture propagation along an antiplane fault in the presence of nonlinear rate-dependent friction. We study rupture dynamics of models with single and twin asperities. In our models, asperities are places on the fault with a higher value of prestress. Othewise all fault parameters are homogeneous. We show that for models with such asperities, a slip velocity weakening friction leads to the propagation of supersonic healing phases and to the spontaneous arrest of fracture if the prestress outside the asperities is low enough. For models with asperities, we can also observe narrow slip velocity pulses, qualitatively similar to the so-called Heaton pulses observed in some earthquake accelerograms. We also observe a complex distribution of stress after the rupture that depends on details of the initial distribution of asperities and on the details of the friction law. 相似文献
17.
本研究基于分层黏弹介质模型,考虑强震或大地震同震位错、震后黏滞松弛及主断层段震间构造应力加载三方面效应,给出1480年以来,川滇菱形块体东边界鲜水河断裂带、安宁河断裂带、则木河断裂带和小江断裂带共20个断层段由三方面效应引起的累积库仑应力变化随时间的演化,分析强震间相互作用和强震发生的应力累积背景,定性分析各断层段的地震危险性.同时,分别采用现今台网地震目录和川滇菱形块体东边界各断层段强震复发间隔两种资料,定量计算2030年各断层段的强震发生概率;并基于摩擦本构理论,将周边强震引起的库仑应力变化量作为应力扰动,修正强震发生概率的计算结果.各断层段累积库仑应力演化的结果表明,鲜水河断裂带中部八美段、色拉哈段及南部磨西段、安宁河断裂带冕宁-西昌段、小江断裂带北部巧家-东川段和南部建水段的累积库仑应力显著增加.修正的强震发生概率计算结果显示,鲜水河断裂带中部八美-色拉哈-康定一带、安宁河断裂带冕宁-西昌段、小江断裂带南部华宁-建水一带强震发生概率较高,地震危险性值得关注.本研究基于库仑应力演化计算定性分析强震危险性的同时,基于摩擦本构律理论,结合地震引起的应力扰动和强震发生背景,定量计算修正的强震发生概率,为川滇菱形块体东边界强震危险地点及中长期发震紧迫程度判定提供方法和依据. 相似文献
18.
本文首先沿走向将鲜水河断裂带划分为炉霍、道孚、乾宁、康定和磨西五个断裂段,利用沿断裂带布设的跨断层短基线、短水准场地测量资料计算了近场的断层活动参数,利用覆盖断裂带相对较大区域的重力、GPS观测资料计算了重力场动态变化、GPS速度场.基于重力场动态变化和GPS速度场采用蚁群算法和粒子群算法(具有全局优化的优势)分别反演计算了五个断裂段断层活动参数,将结果中的走滑分量作为五个断裂段的现今走滑速率.通过对以上三类现今走滑速率及五个断裂段的地质平均滑动速率进行融合与对比分析,将重力资料反演计算结果作为断裂带整体走滑速率,与跨断层短基线、短水准测量计算的断层滑动速率结果进行对比分析,初步判定了各跨断层短基线、短水准场地所跨断裂的性质,最终给出了五个断裂段的现今整体左旋走滑速率和部分分支断裂左旋走滑速率,结果为:(1)炉霍段为9.13mm·a~(-1),虾拉沱区域西支断裂为2.46mm·a~(-1),东支断裂为5.84mm·a~(-1).(2)道孚段为8.57mm·a~(-1),东南段沟普区域西支断裂为1.78mm·a~(-1),东支断裂为6.79mm·a~(-1).(3)乾宁段为7.67mm·a~(-1).(4)康定段为6.14mm·a~(-1).(5)磨西段为4.41mm·a~(-1).本文还定性讨论了断裂带两侧重力、GPS测点覆盖范围内活动地块的三维弹塑性变形和古地震、历史地震造成的永久位错. 相似文献
19.
六棱山北麓断裂新活动特征 总被引：6，自引：1，他引：6
通过对六棱山北麓活动断裂的几何结构、分段活动特征及段落边界等方面的地质地貌调查与研究，认为该活动断裂可分为４段，除东段在早更新世有过活动外，其他３段均为晚更新世晚期～全新世活动段，段落长度１０～３９ｋｍ。该断裂在晚中生代表现为逆冲性质，至新生代随区域构造应力场的变化而转变为倾滑正断层。各段落上垂直位移量分布呈包络线状，而且各段平均滑动速率不同，西大东小，显示断裂新活动强度自西向东变弱 相似文献
20.
FEATURES OF EARTHQUAKE CLUSTERING FROM CALCULATION OF COULOMB STRESS AROUND THE BAYAN HAR BLOCK,TIBETAN PLATEAU 
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下载免费PDF全文 Since 1997, several major earthquakes occurred around the Bayan Har block in the Tibetan plateau, providing an opportunity to further understanding the mechanism of intraplate earthquakes. What is the effect of interactions among these events on the earthquake occurrence pattern is an issue to be addressed. In this article, we use the visco-elastic Coulomb stress changes model to calculate the stress interactions among the historical events close to or large than MS7.0 since 1893 in the Bayan Har block. We apply the relationships between the slip rate and stress accumulation rate to transform the Coulomb stress changes into the influenced time. Then we remove such influence time from the occurrence years, and analyze the effects of the earthquake interactions on the clustering patterns of the historical earthquakes in the Bayan Har block. The results show that the major earthquakes in the Bayan Har block are characterized by a quasi-period of about 16 years from 1893 to 1973 and a clustering occurrence time period from 1997 to present following a relatively long quiescence period. The Bayan Har block is still in the active period with high probabilities of major quakes. We calculate the conditional probabilities of the rupture segments that did not rupture since 1893 of the boundary faults of the Bayan Har block in the next 30 years. The following faults or fault sections seem to be of major risk:The Maqin segment and the Maqu fault of the East Kunlun fault zone, the Awanang fault, the Luocha segment of the Tazhong fault, the Moxi segment of the Xianshuihe fault, and the Dangjiang fault. Other Fault segments in the Bayan Har block without seismic events since 1893 probably also have hazard of MS7 earthquakes in the future. 相似文献