共查询到20条相似文献,搜索用时 156 毫秒
1.
3DstructuralreconstructionofMohointheTangshanearthquakeareabyusinginversionofcurvedinterfaceXIAOLINGLAI(赖晓玲)XIANKANGZHANG... 相似文献
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SomegeologicsignaturesoffaultcrepinthecontinentalareaofChinaHONGFAXIANG(向宏发)SHUNMINGUO(虢顺民)WANXIAZHANG(张晚霞)BINGLIANGZHAN... 相似文献
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InversionofbreakoutdatafrominclinedboreholesforstressstateoftheuppercrustinJizhong depressionYAN-XIANGYU(俞言祥)andZHONG-HUAIXU(... 相似文献
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StudyofCurieisothermalsurfaceinSichuanBasinandtheseismicareaonitswesternmar┐ginXIANZHANG(张先),XI-FENGHU(虎喜凤),JING-XIUSHEN(沈京秀... 相似文献
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Effectsofmagnitudeaccuracyandcomplete┐nesdataonseismichazardparametersHUI-CHENGSHAO(邵辉成),JIA-SHUXIE(谢家树),PINGWANG(王平)andYA-X... 相似文献
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ResearchoninversionofaveragestresfieldbygeneticalgorithmsXING-XINDU(杜兴信)HUI-LINGZHANG(张惠玲)XIU-LINGLU(鲁秀玲)CHUN-SHENGZHANG(张春生... 相似文献
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ElectromagneticefectstimulatedbystrainwaveinrocksXIAOHEXU(徐小荷)GUOJUNXING(邢国军)BIAOWANG(王标)MiningDepartmentofNortheasternUni... 相似文献
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UppermantleflowbeneaththeNorthwestofChinaanditslithosphericdynamicsJIAN-HUAHUANGI(黄建华);XIA-HUACHANGI(常筱华)andRONG-SHANFUI傅容珊)(... 相似文献
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EstimationofseismicstresdropfromthepeakvelocityofgroundmotionJIAZHENGQIN(秦嘉政)ZUYINLIU(刘祖荫)XIAODONGQIAN(钱晓东)QINGYINXIE(谢庆... 相似文献
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Studyonthecharacteristicsofcrust┐mantletransitionzoneinWesternYunnanProvinceHONG-XIANGHU(胡鸿翔)ZHONG-YANGLIN(林中洋)YIN-JUBIAN(边银... 相似文献
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2013年4月20日在四川芦山发生了M S7.0地震,震源运动学反演结果给出了此次地震的破裂过程和同震滑动分布.为了更好地理解造成芦山地震破裂过程的力学原因,本文综合野外地质调查、余震定位、深地震反射剖面等结果,构建芦山地震铲型断层模型,以震源运动学反演结果为约束,将震源参数与震源附近的构造应力场结合,建立断层面上滑动量和牵引力的时空分布关系,通过试错法给定震源动力学计算参数模拟芦山地震破裂传播的可能情况,进而分析讨论不同动力学计算参数对芦山地震破裂过程和同震滑动分布的影响.结果显示,初始应力是决定断层是否发生错动的关键;临界滑动弱化位移D c对破裂滑动速率有着很大的影响;成核区半径和初始应力主要影响破裂成核的快慢;局部不均匀破裂强度主要影响破裂行为和断层最终滑动量分布.利用边界积分方程法可以有效计算芦山地震铲型断层模型的动力学破裂过程,再现此次地震的主要特征.通过探究动力学参数对破裂过程影响,可解释运动学反演结果所揭示的破裂特征的力学原因,对于深入了解地震震源过程的物理本质和预测未来可能发生的地震的主要特征有着重要的参考意义. 相似文献
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本文引入地震序列的一种自扩展模式,其地震序列的发生由地震断层的不同尺度的闭锁段相继破裂而发生,同时给出了以力学参数和几何参数定标的断层的自相似破裂机制,用以解决地震断层的分形特征及破裂的慢化过程。 相似文献
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Using the 78 focal mechanism solutions of the fore shocks, main shock and after shocks of the earthquake sequence for the Yao'an earthquake, the characteristics of the focal faults and stress field for the earthquake sequence are analyzed. The results show that the main rupture plane of the Yao'an earthquake sequence is a tectonic fault with N50°W strike and steep dip and all the main shock, the fore shocks and the vast majority of after shocks occurred on the main rupture plane. A tectonic fracture with NNE-NE strike also participated in development process of the sequence. The focal stress field of the sequence dominated by principal compressional stress with nearly horizontal orientation SSE is consistent with the regional tectonic stress field. In the sequence development, the stress field in the focal region was complex with multi-azimuths and multi-action models and the focal rupture showed complex features with multi-directions and multi-patterns. 相似文献
15.
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
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基于一维单侧有限移动震源模式,根据地震波传播过程中的多普勒效应,分别利用P波和S波拐角频率的方位变化,反演2012年7月20日江苏高邮、宝应交界MS4.9地震的发震断层面参数。P波和S波拐角频率的反演结果一致显示:本次地震的断层面破裂方向为232°左右,破裂面呈NE-SW向;地震马赫数v/c为0.2左右,平均破裂速度小于S波速度,破裂长度较短,为0.2~0.3km左右。破裂面方位与震源机制解、宏观烈度调查和余震精定位的研究结果具有一致性,结合震区周边的地质构造背景,分析认为滁河断裂很可能是高邮、宝应交界MS4.9地震的发震构造。 相似文献
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We propose an inversion scheme for retrieval of characteristics of seismic point sources, which in contrast to common practice,
takes into account anisotropy. If anisotropy is neglected during inversion, the moment tensors retrieved from seismic waves
generated by sources situated in anisotropic media may be biased. Instead of the moment tensor, the geometry of the source
is retrieved directly in our inversion; if necessary, the moment tensor can be then determined from the source geometry aposteriori.
The source geometry is defined by the orientation of the slip vector and the fault normal as well as the strength of the event
given by the size of the slip and the area of the fault. This approach allows direct interpretation of the source geometry
in terms of shear and tensile faulting. It also makes possible to identify volumetric source changes that occur during rupturing.
We apply the described algorithm to one event of the 2000 West Bohemia earthquake swarm episode. For inversion we use information
of the direct P waves. The structure is approximated by three different models determined from travel-time observations. The
models are inhomogeneous isotropic, inhomogeneous anisotropic, and homogeneous anisotropic. For these models we obtain seismic
moments MT = 3.2 − 3.8 × 1014 Nm and left-lateral near-vertical oblique normal faulting on a N-S trending rupture surface. The orientation of the rupture
surface is consistent with fault-plane solutions of earlier studies and with the spatial distribution of other events during
this swarm. The studied event seems to be accompanied by a small amount of crack opening. The amount of crack opening is slightly
reduced when the inhomogeneous anisotropic model is assumed, but it persists. These results and additional independent observations
seem to indicate that tensile faulting occurs as a result of high fluid pressure. 相似文献
18.
本文在Asperity模式和Barrier模式的基础上,提出了另外一种不均匀体模式——障碍体模式,并对该模式进行了数值模拟的研究。结果除证实了我们以前做过的单轴压力下模拟障碍体的实验结果以外,还表明在含有障碍体的断层面上,破裂的扩展与破裂的传播速度、始破裂区域的大小、裂纹的类型以及障碍体所在断层的介质有关。在有围压的情况下,破裂可以先越过或绕过强度较高或尺度较大的障碍体,经一段时间的应力积累过程后,再使障碍体发生破坏。本文通过对震源区中障碍体的性质和影响的研究,解释了海城和邢台两个地震序列形成和发展的可能原因,得到一些较为合理的结果。 相似文献
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A long sequence of earthquakes causing few casualties and considerable damage in a wide zone struck Central Italy starting on September 26, 1997. Theearthquakes are characterized by normal faulting mechanism, with a NE-SW(anti-Apenninic direction) tension axis. In this paper we analyze the accelerometric recordings collected by the accelerograph stations belonging to the National Accelerograph Network. About 10 stations were triggered by the mainshocks of the sequence. In particular, a small size foreshock and the two mainshocks that occurred on September,26 (00:33(GMT) MW = 5.7 and 09:40 MW = 6.0) have been recorded by two digital 3-C accelerometers located at near source distances (within 30 km from the faults). These records are relevant to investigate the detail of therupture kinematics, due to the close epicentral distance and azimuthallocation relative to the fault orientation and geometry. Using a trial and error approach we modeled the source mechanism through the fit of the arrival times, the apparent source time duration, the main polarization features and the entire waveforms of the recorded signals, in order to get some insight on the rupture evolution, the location of the fracture origin point and the fault geometry. Based on this fault kinematic model, inferences on fault slip distribution are obtained by modeling the S acceleration waveform, comparing the ray theory synthetics with 1–5 Hz band filtered ground velocity records.The final model shows that the seismic ruptures occurred along two adjacent,sub-parallel, low angle dipping normal faults. Ruptures bothnucleated from the fault bottom and propagated up-dip, showing differentrupture velocity and length. The presence of a transfer zone (barrier)can be suggested by the mainshocks rupture evolution. This transfer zonehas probably controlled the amplitude increase of local stressreleased by the first rupture at its NW edge which triggered about 9 hourslater the second rupture. The inferred model was used to compute the predictedground acceleration in the near source range, using a hybridstatistical-deterministic approach.A similar trial and error method has been also applied to the October 14, 199715:23 earthquake (MW = 5.6). The inferred kinematic model indicates a rupture nucleating from the faultbottom and propagating up-dip, toward the SE direction. Thus the three mainshocks ruptured distinct fault segments, adjacent and slightly offsetfrom one to another. 相似文献