数字地震数据的处理研究—真实地面运动的复原   总被引：2，自引：1，他引：2  

何少林  李海亮 《地震地磁观测与研究》1997,18(6):52-58

讨论了在频域中真实地面运动的复原问题，借助于一个稳定的六阶带通滤波器可使地震仪反演系统趋于稳定，最后由关分方程递归求出真实地动位移，结果表明，对同一个地震，不同的仪器其原始响应不同，但由其复原的真实地面运动结果却有相当好的一致性。这证明了所采用的复原方法的可用性。  相似文献   

Analysis and study of the large earthquake risk in Yanqing-Huailai basin     

刘昌铨  嘉世旭  刘明军  李长发 《地震学报(英文版)》1997,10(5):639-647

ＡｎａｌｙｓｉｓａｎｄｓｔｕｄｙｏｆｔｈｅｌａｒｇｅｅａｒｔｈｑｕａｋｅｒｉｓｋｉｎＹａｎｑｉｎｇＨｕａｉｌａｉｂａｓｉｎＣＨＡＮＧＱＵＡＮＬＩＵ（刘昌铨）ＳＨＩＸＵＪＩＡ（嘉世旭）ＭＩＮＧＪＵＮＬＩＵ（刘明军）ＣＨＡＮＧＦＡＬＩ（李长发...  相似文献   

四川地区强震发生条件的综合分析   总被引：2，自引：0，他引：2  

黄祖智  唐荣昌 《地震研究》1997,20(2):185-192

根据发震断层的时代，发震构造的应力和几何结构条件，对四川地区的强震发生条件进行了综合分析，结果表明，四川地区孕育和发生强震的断层主要晚更新世以来，特别是全新世以来活动的断裂；强震多发生在主压力方向与断层交角成３０°～６０°之间的最危险滑动角值范围，走滑断层的斜列状结构，断裂的交叉结构，断裂的枢纽结构，断裂上的弯曲，转折部位以及断裂带上的横向隆起，拗陷及其交接部位都是发震构造的结构特征，有利于强震的  相似文献   

根据i—f—j模式估计山西平陆地区的长期强震潜势     

胡先明 《地震研究》1997,20(2):193-198

山西省平陆地区位于山西地震带南端，为了分析该地区未来的长期强需求潜势，本较系统地分析当地的破坏性地震及１５００年以来的有地震地震资料，并进一步应用中国在陆特征的地震轮回模式及其复发时间概率模型估算法当前特征地震轮回的平均时间间隔，以及从１９９５年起未来百年内复发强震的概率，结果表明：未来１００年来该地区复发强震的危险性很高，未来５０年内复发强震的危险性也不能排除。  相似文献   

唐山地震的超晚期强余震估计   总被引：1，自引：0，他引：1  

戴英华  李淑莲 《华北地震科学》1997,15(4):1-9

根据华北历史地震的重复性和免疫性，认为在唐山周围８５ｋｍ，２００年内，对６级地震具有一定的免疫性；在研究了唐山地震序列自身的衰减规律后，认为在今后几十几强余震的最大活动水平为５级，发生６级以上土地震的可能性很小。  相似文献   

地下水宏观异常与强震临震预报     

李坤  李秀英 《华北地震科学》1997,15(4):57-63

阐述了如何利用地下水宏观异常作强烈地震的临震预报，详细叙述了利用地下水宏观异常预报地震三要素的方法。  相似文献   

中强地震前油井动态异常机理研究   总被引：1，自引：0，他引：1  

李一兵  张德元 《华北地震科学》1997,15(4):64-72

在分析油井映震特征的基础上，着重对油井动态异常的形成机理进行了研究。认为：映震灵敏井孔的空间分布主要受应力易于集中的构造条件的控制，特别是断层的又汇处、转折端和断裂带，这是与其他流体观测项目的相同之处；在本研究中，首次提出了油井动态前兆异常形成的三种力学过程，即岩土力学过程、水动力学过程和气体动力学过程以及油井特有的二种”放大”作用（变径和气体膨胀）的观点；解释了油井动态震前多为正异常的力学机制。  相似文献   

热力强迫对越赤道气流产生和维持的作用——定性分析     

王向东  廖洞贤 《气象学报》1997,55(4):484-491

从原始方程出发，应用大气运动的对称反对称性理论，就赤道地区一呈偶极子分布的反对称冷热源对越赤道气流的形成和维持作用进行了定性分析。结果表明，非绝热加热的反对称分布对越赤道气流的影响是通过诱发和维持反对称的气压场分量来实现的。即在热源上空低层形成低压，高层形成高压；在热汇上空形成相反的气压场。这样，在赤道上空高、低层就将形成与相应气压梯度方向一致的越赤道气流  相似文献   

The glacilacustrine sedimentary environment of Bowser Lake in the northern Coast Mountains of British Columbia, Canada     

Robert Gilbert  Joseph R. Desloges  John J. Clague 《Journal of Paleolimnology》1997,17(3):331-346

Bowser Lake, a fiord lake in the northern Coast Mountains of British Columbia, contains a thick Holocene fill consisting mainly of silt and clay varves. These sediments were carried into the lake by proglacial Bowser River which drains a high-energy, heavily glacierized basin. Sedimentation in the lake is controlled by seasonal snow and ice melt, by autumn rainstorms, and by rare, but very large jökulhlaups from glacier-dammed lakes in the upper Bowser River basin which complicate environmental inferences from the sedimentary record. Sediment is dispersed through the deep western part of the lake by energetic turbidity currents. The turbidity currents apparently do not overtop a sill that separates the western basin from much shallower areas to the east. Large amounts of silt and clay are deposited from suspension in the eastern part of the lake, but sediment accumulation rates there are much lower than to the west. Several strong acoustic reflectors punctuate the varved fill in the western basin; these may be thick or relatively coarse beds deposited during jökulhlaups or exceptionally large storms. The contemporary sediment yield to Bowser Lake, estimated from sediments in the lake, is about 360 t km^-2a^-1. This is a relatively high value, but it is less than yields insome other, similar montane basins with extensive snow and ice cover.The most likely explanation for the difference is that large amounts of sediment have been, and continue to be, stored on the Bowser delta andin small proglacial lakes.  相似文献   

The Zihuatanejo, Mexico, earthquake of 1994 December 10 (M= 6.6): source characteristics and tectonic implications     

M. Cocco  J. Pacheco  S. K. Singh  F. Courboulex 《Geophysical Journal International》1997,131(1):135-145

An analysis of the Zihuatanejo, Mexico, earthquake of 1994 December 10 ( M = 6.6), based on teleseismic and near-source data, shows that it was a normal-faulting, intermediate-depth ( H = 50 ± 5 km) event. It was located about 30 km inland, within the subducted Cocos plate. The preferred fault plane has an azimuth of 130°, a dip of 79° and a rake of −86°. The rupture consisted of two subevents which were separated in time by about 2 s, with the second subevent occurring downdip of the first. The measured stress drop was relatively high, requiring a Δσ of about a kilobar to explain the high-frequency level of the near-source spectra. A rough estimate of the thickness of the seismogenic part of the oceanic lithosphere below Zihuatanejo, based on the depth and the rupture extent of this event, is 40 km.
This event and the Oaxaca earthquake of 1931 January 15 ( M = 7.8) are the two significant normal-faulting, intermediate-depth shocks whose epicentres are closest to the coast. Both of these earthquakes were preceded by several large to great shallow, low-angle thrust earthquakes, occurring updip. The observations in other subduction zones show just the opposite: normal-faulting events precede, not succeed, updip, thrust shocks. Indeed, the thrust events, soon after their occurrence, are expected to cause compression in the slab, thus inhibiting the occurrence of normal-faulting events. To explain the occurrence of the Zihuatanejo earthquake, we note that the Cocos plate, after an initial shallow-angle subduction, unbends and becomes subhorizontal. In the region of the unbending, the bottom of the slab is in horizontal extension. We speculate that the large updip seismic slip during shallow, low-angle thrust events increases the buckling of the slab, resulting in an incremental tensional stress at the bottom of the slab and causing normal-faulting earthquakes. This explanation may also hold for the 1931 Oaxaca event.  相似文献