马衔山北缘断裂西段6.5级地震对兰州市及周边地区的影响
详细信息 本馆镜像全文    |  推荐本文 | | 获取馆网全文
摘要
位于兰州市南侧NW走向的马衔山北缘断裂是发生强烈地震最危险的地段。本文采用混合震源模型和随机合成高频地震动方法,研究了该断裂西段发生6.5级地震可能引起的兰州市及周边地区的地震动分布,给出了PGA分布图。
The Maxianshan north margin fault with strike NW crossing through south of Lanzhou city is the most dangerous place for a future strong earthquake to the city.Using the hybrid source model and the method of stochastic synthesizing high-frequency ground motion,the strong ground motion field in Langzhou city and its vicinity from an earthquake with magnitude 6.5 on the western segment of the fault is forecasted in this paper,the spatial characteristics and pattern of the field is summarized.
引文
[1]中华人民共和国国家标准.建筑物抗震设计规范(BG50011-2001)[S].北京:中国建筑工业出版社,2002.
    [2]陶夏新,李小军.工程地震基本科学问题[A]∥国家自然科学基金委员会工程与材料科学部.学科发展战略研究报告(2006年—2010年),建筑、环境与土木工程II(土木工程卷)[G].北京:科学出版社,2006:367-381.
    [3]D MBoore.Comparisons of Ground Motions from the 1999 Chi-Chi Earthquake with Empirical Predictions Largely Based on Datafrom California[J].Bulletin of the Seismological Society of Ameri-ca,2001,91(5):1212-1217.
    [4]X X Tao,J G Anderson.Near field strong ground motion simula-tion[A]∥Proceeding of International Conference on Advancesand New Challenges in Earthquake Engineering Research[C].Harbin.2002.
    [5]TKhosrow,K TShabestari,F Yamazaki.Near-fault spatial varia-tion in strong ground motion due to rupture directivity and hangingwall effects from the Chi-Chi,Taiwan earthquake[J].Earth-quake Engineering and Structure Dynamic,2003,32(14):2197-2219.
    [6]HKawase.The cause of the damage belt in Kobe:"the basin-edge effect"constructive interference of the direct S wave with thebasin induced diffracted/Rayleigh waves[J].Bulletin of the Seis-mological Society of America,1996,67(1):25-34.
    [7]I A Beresenv,G Atkinson.Stochastic finite-fault modeling ofground motions from the 1994 Northridge,California,earth-quake,I.Validation on rock sites[J].Bulletin of the Seismolog-ical Society of America,1998,88(6):1392-1401.
    [8]I ABeresenv,G Atkinson.Generic finite-fault model for ground-motion prediction in Eastern North America[J].Bulletin of theSeismological Society of America,1999,89(3):608-625.
    [9]X X Tao,G X Wang.Rupture directivity and hanging wall effectin near field strong ground motion simulation[J].ACTA Seis-mologica Sinica,2003,16(2):205-212.
    [10]X X Tao,H Y Wang.A random source model for near filedstrong ground motion prediction[A]∥Proceeding of the 13thWorld Conference on Earthquake Engineering[C].Vancouver,Canada,2004.
    [11]H Y Wang,X X Tao,J Li.Global source parameters of finitefault model for strong ground motion predictions[A]∥Proceed-ing of the 13th World Conference on Earthquake Engineering[C].Vancouver,Canada,2004.
    [12]王海云,陶夏新.近场强地震动预测中浅源地震的Asperity模型特征[J].哈尔滨工业大学学报,2005,37(11):1533-1539.
    [13]HY Wang,X X Tao.Relationships between moment magnitudeand fault parameters:theoretical and semi-empirical relations[J].Earthquake Engineering and Engineering Vibration,2003,2(2):201-211.
    [14]孙晓丹.震源对大跨度空间结构地震动输入的影响[D].哈尔滨工业大学,2005.
    [15]HKanamori,D L Anderson.Theoretical basis of some empiricalrelations in seismology[J].Bulletin of the Seismological Societyof America,1975,65(5):1073-1095.
    [16]王海云.近场强地震动预测的随机震源模型[D].中国地震局工程力学研究所,2004.
    [17]T C Hanks,R K McGuire.The character of high-frequencystrong ground motion[J].Bulletin of the Seismological Societyof America,1981,71(6):2071-2095.
    [18]G Atkinson,D M Boore.Stochastic point source modeling ofground motion in the Cascadia region[J].Seismological Re-search Letter.1997,68(1):74-85.
    [19]G Atkinson,W Silva.An empirical study of earthquake sourcespectra for California earthquakes[J].Bulletin of the Seismologi-cal Society of America,1997,87(1):97-113.
    [20]G Atkinson,W Silva.Stochastic Modeling of California groundmotions[J].Bulletin of the Seismological Society of America,2000,90(2):255-274.
    [21]I A Beresenv,G Atkinson.Modeling finite-fault radiation fromtheωnspectrum[J].Bulletin of the Seismological Society of A-merica,1997,87(1):67-84.
    [22]K Aki.Scaling lawof seismic spectrum[J].Journal of Geophysi-cal Research,1967,72:1212-123.1
    [23]TC Hanks.bvalues andω2seismic source models:implicationsfor tectonic stress variation along active crustal fault zones and theestimation of high-frequency strong ground motion[J].Journal ofGeophysical Research,1979,84(5):2235-2242.
    [24]J G Boatwright,G L Choy.Acceleration source spectra anticipa-ted for large earthquakes in northeastern North America[J].Bul-letin of the Seismological Society of America,1992,82(2):660-682.
    [25]G Atkinson.Earthquake source spectra in the Eastern North A-merica[J].Bulletin of the Seismological Society of America,1993,83(6):1778-1798.
    [26]G Atkinson,D M Boore.Evaluation of models for earthquakesource spectra in eastern North America[J].Bulletin of the Seis-mological Society of America,1998,88(4):917-934.
    [27]I A Beresenv,G Atkinson.Source parameters of earthquakes ineastern and western North America based on finite-fault modeling[J].Bulletin of the Seismological Society of America,2002,92(2):695-710.
    [28]D Motazedian,G M Atkinson.Stochastic Finite-Fault ModelingBased on a Dynamic Corner Frequency[J].Bulletin of the Seis-mological Society of America,2005,95(3):995-1010.
    [29]B Mohammadioum,L Serva.Stress drop,slip type,earthquakemagnitude,and seismic hazard[J].Bulletin of the SeismologicalSociety of America,2001,91(4):694-707.
    [30]孙崇绍.西北黄土地区河谷城市地震动参数小区划研究———以兰州为例[J].西北地震学报,2007,29(1):1-11.
    [31]尹志文,许健生,李苹.永登5.8级地震前后小震的震源参数和介质Q值变化特征研究[J].西北地震学报,1999,20(4):14-20.

版权所有:© 2023 中国地质图书馆 中国地质调查局地学文献中心