丽江地震前后重力场变化的有限矩形位错模型分析   总被引：1，自引：0，他引：1       下载免费PDF全文

燕乃玲  李辉  申重阳 《地震学报》2003,25(2):172-181

研究了用有限矩形位错模型计算地壳形变引起的地面重力场变化的方法．以丽江MＳ7.0地震为例，讨论了确定用于模型计算的断层面参数的原则，并给出了结果．计算和分析了不同类型位错引起的重力场变化图象特征，并与丽江地震前后观测到的重力场变化进行比较．结果表明，在发震断层有限范围内模型可解释同震重力场的变化，但模型对于更大空间范围上的重力场变化并不能给出很好地解释.   相似文献   

丽江地震序列的震源机制,发震应力场和破裂特征   总被引：17，自引：5，他引：17  

王绍晋  罗淑进 《地震研究》1997,20(1):26-34

丽江７．０级地震震区位于我国西南地区现代构造应力场空间分布的复杂地区，区域应力场主压应力优势方位为南南东。震区位于可能受到多种构造动力源作用的特定构造运动环境中。获得了主震和２２个ＭＬ≥４．０级余震的震源机制Ｐ波初动解，分析表明，主震发震应力场为北３°东，与震区区域应力场主压应力优势方位有一个小角度的偏差。主震的发震应力不仅有水平应力的作用，同时还有显的垂直应力的作用。在余震序列发展中震区呈现出  相似文献   

1996年阿图什6.9级地震参数与宏观震中   总被引：5，自引：0，他引：5  

杨成荣 《内陆地震》1997,11(2):154-159

对通过计算机定位得到１９９６年３月１９日阿图什６．９级地震基本参数的可靠性进行了分析与论证，并对该次地震微观震中与宏观震中差异较大的原因进行了探讨。  相似文献   

Dynamic nucleation process of shallow earthquake faulting in a fault zone     

Nobuki Kame  Teruo Yamashita 《Geophysical Journal International》1997,128(1):204-216

Two distinct phases are commonly observed at the initial part of seismograms of large shallow earthquakes: low-frequency and low-amplitude waves following the onset of a P wave ( P ₁) are interrupted by the arrival of the second impulsive phase P₂ enriched with high-frequency components. This observation suggests that a large shallow earthquake involves two qualitatively different stages of rupture at its nucleation.
We propose a theoretical model that can naturally explain the above nucleation behaviour. The model is 2-D and the deformation is assumed to be anti-plane. A key clement in our model is the assumption of a zone in which numbers of pre-existing cracks are densely distributed; this cracked zone is a model for the fault zone. Dynamic crack growth nucleated in such a zone is intensely affected by the crack interactions, which exert two conflicting effects: one tends to accelerate the crack growth, and the other tends to decelerate it. The accelerating and decelerating effects are generally ascribable to coplanar and non-coplanar crack interactions, respectively. We rigorously treat the multiple interactions among the cracks, using the boundary integral equation method (BIEM), and assume the critical stress fracture criterion for the analysis of spontaneous crack propagation.
Our analysis shows that a dynamic rupture nucleated in the cracked zone begins to grow slowly due to the relative predominance of non-coplanar interactions. This process radiates the P₁ phase. If the crack continues to grow, coalescence with adjacent coplanar cracks occurs after a short time. Then, coplanar interactions suddenly begin to prevail and crack growth is accelerated; the P₂ phase is emitted in this process. It is interpreted that the two distinct phases appear in the process of the transition from non-coplanar to coplanar interaction predominance.  相似文献   

区域-时间-长度算法及其在华北中强地震中短期前兆特征研究中的应用   总被引：5，自引：1，他引：5       下载免费PDF全文

蒋海昆  侯海峰  周焕鹏  周翠英 《地震学报》2004,26(2):151-161

引入并改进了区域-时间-长度算法（region-time-length algorithm），较之原来的定义更加强调了地震破裂尺度函数对VRTL的贡献，同时保证了震中距函数、时间函数及破裂尺度函数对VRTL影响的权系数相等．华北5级以上地震的回顾性预测研究结果表明，改进的RTL算法所得到的异常大多具有短期或中短期特征. 震前VRTL变化型态可分为两类:Ⅰ类具有相对完整的变化形态，大多呈现从0开始的上升——转折下降或下降——转折上升形态；Ⅱ类变化形态不完整，一般从0开始急剧上升或下降，无明显转折，主震发生在VRTL极值附近．VRTL上升表征地震活动水平相对于背景变化率的增高，意味着地震活动增强；VRTL下降则意味着地震活动相对于背景变化率的降低，在一定程度上表征了地震活动的平静．据此给出由RTL算法进行中、短期异常识别并粗略估计发震时间的方法. 该方法Ⅰ,Ⅱ类异常3个月内发震的R值评分分别为0.6及0.3左右， 6个月内的R评分分别为0.7及0.4左右．对特征时间跨度、特征距离、震级下限等对VRTL的影响, 以及其它一些实际应用中的重要问题进行了初步讨论．   相似文献   

Physical interpretation of the breakdown process using a rate- and state-dependent friction law     

M. Cocco  A. Bizzarri  E. Tinti 《Tectonophysics》2004,378(3-4):241

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Rupture process of the 1999 November 12 Düzce (Turkey) earthquake deduced from strong motion and Global Positioning System measurements     

M.-P. Bouin  M. Bouchon  H. Karabulut  M. Aktar 《Geophysical Journal International》2004,159(1):207-211

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Structural and geotechnical impacts of surface rupture on highway structures during recent earthquakes in Turkey   总被引：4，自引：0，他引：4  

A. Pamuk  E. Kalkan  H.I. Ling 《Soil Dynamics and Earthquake Engineering》2005,25(7-10):581-589

The most significant damage on highway bridges during the recent earthquakes in Turkey (Kocaeli and Duzce earthquakes) and Taiwan (Chi–Chi earthquake) was the result of fault ruptures traversing transportation infrastructure. This phenomenon and its consequences accentuate the need to examine surface rupture hazards and to identify those areas at risk. This understanding can help to develop remedial measures for both structural and geotechnical engineering. For that purpose, damage to highway bridges during the recent events was reviewed. The total collapse of the highway overpass in Arifiye, during the Kocaeli earthquake, was investigated. The major problems under consideration (in Arifiye) were: (i) dislodging of the bridge spans, and consequently, the total separation of the reinforced concrete girders from the piers; and (ii) the stability of a mechanically stabilized earth wall (MSEW) system under extreme loading conditions. The results of the structural and geotechnical investigations presented herein can be taken in consideration to improve transportation infrastructure against surface rupture hazards.  相似文献   

Numerical simulation for 1975 Haicheng and 1999 Xiuyan earthquake processes by DDA+FEM     

张瑞青  魏富胜  乔成斌  林邦慧 《地震学报(英文版)》2005,18(2):171-179

Introduction The Xiuyan earthquake(MS=5.4)on Nov.29,1999,occurred between Hushan town and Pi-anling town at the southeast end of the aftershocks of Haicheng earthquake(MS=7.3).These two earthquakes′sequences are highly similar in the way that the foreshocks are very frequent,focal mechanisms of the main shocks are about the same and fault strikes are approximately in the same direction.It is important to study these earthquakes for further research on seismogenesis to fore-cast earthquake…  相似文献   

Creation of the Cocos and Nazca plates by fission of the Farallon plate   总被引：4，自引：0，他引：4  

Peter Lonsdale   《Tectonophysics》2005,404(3-4):237-264

Throughout the Early Tertiary the area of the Farallon oceanic plate was episodically diminished by detachment of large and small northern regions, which became independently moving plates and microplates. The nature and history of Farallon plate fragmentation has been inferred mainly from structural patterns on the western, Pacific-plate flank of the East Pacific Rise, because the fragmented eastern flank has been subducted. The final episode of plate fragmentation occurred at the beginning of the Miocene, when the Cocos plate was split off, leaving the much reduced Farallon plate to be renamed the Nazca plate, and initiating Cocos–Nazca spreading. Some Oligocene Farallon plate with rifted margins that are a direct record of this plate-splitting event has survived in the eastern tropical Pacific, most extensively off northern Peru and Ecuador. Small remnants of the conjugate northern rifted margin are exposed off Costa Rica, and perhaps south of Panama. Marine geophysical profiles (bathymetric, magnetic and seismic reflection) and multibeam sonar swaths across these rifted oceanic margins, combined with surveys of 30–20 Ma crust on the western rise-flank, indicate that (i) Localized lithospheric rupture to create a new plate boundary was preceded by plate stretching and fracturing in a belt several hundred km wide. Fissural volcanism along some of these fractures built volcanic ridges (e.g., Alvarado and Sarmiento Ridges) that are 1–2 km high and parallel to “absolute” Farallon plate motion; they closely resemble fissural ridges described from the young western flank of the present Pacific–Nazca rise. (ii) For 1–2 m.y. prior to final rupture of the Farallon plate, perhaps coinciding with the period of lithospheric stretching, the entire plate changed direction to a more easterly (“Nazca-like”) course; after the split the northern (Cocos) part reverted to a northeasterly absolute motion. (iii) The plate-splitting fracture that became the site of initial Cocos–Nazca spreading was a linear feature that, at least through the 680 km of ruptured Oligocene lithosphere known to have avoided subduction, did not follow any pre-existing feature on the Farallon plate, e.g., a “fracture zone” trail of a transform fault. (iv) The margins of surviving parts of the plate-splitting fracture have narrow shoulders raised by uplift of unloaded footwalls, and partially buried by fissural volcanism. (v) Cocos–Nazca spreading began at 23 Ma; reports of older Cocos–Nazca crust in the eastern Panama Basin were based on misidentified magnetic anomalies.There is increased evidence that the driving force for the 23 Ma fission of the Farallon plate was the divergence of slab-pull stresses at the Middle America and South America subduction zones. The timing and location of the split may have been influenced by (i) the increasingly divergent northeast slab pull at the Middle America subduction zone, which lengthened and reoriented because of motion between the North America and Caribbean plates; (ii) the slightly earlier detachment of a northern part of the plate that had been entering the California subduction zone, contributing a less divergent plate-driving stress; and (iii) weakening of older parts of the plate by the Galapagos hotspot, which had come to underlie the equatorial region, midway between the risecrest and the two subduction zones, by the Late Oligocene.  相似文献