中国大陆地震(M_s≥6.0)震中与其发震断层距离的统计分析及其在确定潜在震源区边界中的应用     

胡银磊  张裕明  董瑞树  周本刚  冉洪流 《中国地震》1996,(2)

本文通过中国大陆地震(M≥6.0)震中与其发震断层的距离的统计与分析,认为该距离的分布基本上符合正态分布特征,并经拟合计算得到中国东部和西部地区不同类型断层上不同震级档的地震震中距离分布的期望值和方差。根据正态分布随机变量的区间估计方法,讨论了统计分析的结果在潜在震源区边界的确定、以及边界的不确定性评价中的应用。  相似文献   

Aseismio fault slip and block deformation in North China   总被引：1，自引：0，他引：1  

Lanbo Liu  Alan T. Linde  I. Selwyn Sacks  Shihai He 《Pure and Applied Geophysics》1996,146(3-4):717-740

In North China, the tectonic fault-block system enables us to use the Discontinuous Deformation Analysis (DDA) method to simulate the long-term cross-fault survey and other geodetic data related to aseismic tectonic deformation. By the simulation we have found that: (1) Slips on faults with different orientation are generally in agreement with the ENE-WSW tectonic stress field, but the slip pattern of faulting can vary from nearly orthogonal, to pure shear along the strike of the faults, this pattern cannot be explained by simple geometric relation between the strike of the fault and the direction of the tectonic shortening. This phenomenon has been observed at many sites of cross-fault geodetic surveys, and might be caused by the interactions between different blocks and faults. (2) According to the DDA model, if the average aseismic slip rate along major active faults is at the order of several tenths of millimeter per year as observed by the cross-fault geodetic surveys, the typical strain rate inside a block is at the order of 10^–8 year^–1 or less, so that the rate of 10^–6 year^–1, as reported by observations in smaller areas, cannot be the representative deformation rate in this region. (3) Between the slips caused by regional compression and block rotation, there is a possibility that the sense of slip caused by rigid body rotation in two adjacent blocks is opposite to the slip caused by the tectonic compression. But the magnitude of slip resulting from the tectonic compression is much larger than that due to the block rotation. Thus, in general, the slip pattern on faults as a whole agrees with the sense of tectonic compression in this region. That is to say, the slip caused by regional compression dominates the entire slip budget. (4) Based on (3), some observed slips in contradiction to ENE tectonic stress field may be caused by more localized sources, and have no tectonic significance.  相似文献   

灰色关联分析在预测铀成矿断裂中的应用     

祝民强  周俐麟 《华东地质学院学报》1996,19(3):242-246

本文在总结苗儿山岩体中段铀矿田成矿断裂构造特点的基础上，应用灰色系统理论，分析了该地区３７条主要硅化断裂带的成矿条件，并对其找矿的远景进行判别和优选，取得了较好效果。  相似文献   

印尼中加里曼丹波拉湾煤勘探区的构造解析     

杨雄庭  王泽安 《湖南地质》1996,15(4):234-238

本文从区域构造背景出发，根据波拉湾煤勘探区地表及钻孔资料综合分析，建立了逆冲断层Ｆ１、Ｆ２及其配套的ｆ１、ｆ２……构造，理顺了错综复杂的构造格局，将推覆构造理论成功地用于援外生产实践。  相似文献   

青藏高原北缘新构造运动特征     

唐哲民  崔军文 《新疆地质》1996,(3)

ＮＥＥ向阿尔金主断裂带的新构造运动以左旋压扭性活动为特征，仅西端发育张性构造，并可划分出两期变形，新构造运动强度在时间上自上新世晚期开始至第四纪断裂活动强度增大，在空间上自ＳＷＷ向ＮＥＥ方向断裂活动强度逐渐减弱；柴达木北缘的新构造运动可划分为两期，其主要构造特征表现为向柴达木盆地逆冲的前进式叠瓦道冲带，柴达木盆地第四纪时的北界相对于第三纪时的北界向南迁移了数十公里；河西走廊盆地的新构造运动主要表现为盆地边缘断裂的逆冲兼走滑，盆地接受新生代沉积、盆地内第三系的轴面南倾的褶皱；ＮＥＥ向阿尔金主断裂带与其南侧的ＮＷＷ向断裂带是在统一构造应力场作用下相互协调、同时活动的两组关系紧密的构造带，两者的共同活动构成了断块运动。  相似文献   

乌鲁木齐西山断层新构造运动特征   总被引：4，自引：0，他引：4  

胡军  栾超群  胡方秋  郑福婉  南凌  蔡仲琼 《新疆地质》1996,(3)

展布于哈萨克斯坦—准噶尔亚板块南缘西山南麓的乌鲁木齐西山断层，构造地貌发育，航卫片上线性影象清晰，呈舒缓波状。断面倾向ＮＷＷ，倾角６０°～８３°。破碎带宽约１００ｍ，内含多个断面，构成叠瓦状构造，逆冲量颇大。在走向近ＮＥ区段有一定左行走滑活动分量。新构造运动使侏罗系逆冲到中更新统之上，断层断错了全新统的冲积层。由中强地震沿西山断层分布资料显示，现今仍为粘滑活动。经１４Ｃ测年确定，最近两次明显粘滑活动时间为４７５９ａ和４９３ａ，其时间间隔为４２６６ａ，其中一个断面的逆冲量分别为１．０ｍ和０．２５ｍ。  相似文献   

NW断裂构造──鹅公山火山盆地铀矿成矿的关键要素     

张万良 《铀矿地质》1996,(2)

鹅公山火山盆地受郯庐断裂系影响，ＮＷ断裂构造尤为特色：张扭性，倾向ＮＥ，右行下滑，对盆地中３个铀矿床及绝大多数铀矿（化）点具明显控制作用，是铀矿成矿的关键要素。研究ＮＷ断裂对在鹅公山火山盆地及其它地区找矿都具有实际意义。  相似文献   

南京湖山地区棒锤山纵向断层的发现及其地质意义     

杜国云 《江苏地质》1996,20(1):57-58

作者在野外数学中发现，棒锤山人工露头上存在一条重要的纵向断层，经研究认为、棒锤山纵向断层反映了汤－仑推覆体在其发展中至少存在两次明显的应力释放过程，它可能与两次大的构造推覆及应力集中有关。  相似文献   

Instability model for recurring large and great earthquakes in southern California     

William D. Stuart 《Pure and Applied Geophysics》1984,122(6):793-811

The locked section of the San Andreas fault in southern California has experienced a number of large and great earthquakes in the past, and thus is expected to have more in the future. To estimate the location, time, and slip of the next few earthquakes, an earthquake instability model is formulated. The model is similar to one recently developed for moderate earthquakes on the San Andreas fault near Parkfield, California. In both models, unstable faulting (the earthquake analog) is caused by failure of all or part of a patch of brittle, strain-softening fault zone. In the present model the patch extends downward from the ground surface to about 12 km depth, and extends 500 km along strike from Parkfield to the Salton Sea. The variation of patch strength along strike is adjusted by trial until the computed sequence of instabilities matches the sequence of large and great earthquakes sincea.d. 1080 reported by Sieh and others. The last earthquake was theM=8.3 Ft. Tejon event in 1857. The resulting strength variation has five contiguous sections of alternately low and high strength. From north to south, the approximate locations of the sections are: (1) Parkfield to Bitterwater Valley, (2) Bitterwater Valley to Lake Hughes, (3) Lake Hughes to San Bernardino, (4) San Bernardino to Palm Springs, and (5) Palm Springs to the Salton Sea. Sections 1, 3, and 5 have strengths between 53 and 88 bars; sections 2 and 4 have strengths between 164 and 193 bars. Patch section ends and unstable rupture ends usually coincide, although one or more adjacent patch sections may fail unstably at once. The model predicts that the next sections of the fault to slip unstably will be 1, 3, and 5; the order and dates depend on the assumed length of an earthquake rupture in about 1700.  相似文献   

Anomalous hydrogen emissions from the San Andreas fault observed at the Cienega Winery,central California     

Motoaki Sato  A. J. Sutton  K. A. McGee 《Pure and Applied Geophysics》1984,122(2-4):376-391

We began continuous monitoring of H₂ concentration in soil along the San Andreas and Calaveras faults in central California in December 1980, using small H₂/O₂ fuel-cell sensors. Ten monitoring stations deployed to date have shown that anomalous H₂ emissions take place occasionally in addition to diurnal changes. Among the ten sites, the Cienega Winery site has produced data that are characterized by very small diurnal changes, a stable baseline, and remarkably distinct spike-like H₂ anomalies since its installation in July 1982. A major peak appeared on 1–10 November 1982, and another on 3 April 1983, and a medium peak on 1 November 1983. The occurrences of these peaks coincided with periods of very low seismicity within a radius of 50 km from the site. In order to methodically assess how these peaks are related to earthquakes, three H₂ degassing models were examined. A plausible correlational pattern was obtained by using a model that (1) adopts a hemicircular spreading pattern of H₂ along an incipient fracture plane from the hypocenter of an earthquake, (2) relies on the FeO–H₂O reaction for H₂ generation, and (3) relates the accumulated amount of H₂ to the mass of serpentinization of underlying ophiolitic rocks; the mass was tentatively assumed to be proportional to the seismic energy of the earthquake.  相似文献