Effects of Fault Dip and Slip Rake Angles on Near-Source Ground Motions: Why Rupture Directivity Was Minimal in the 1999 Chi-Chi, Taiwan, Earthquake
暂无分享,去创建一个
[1] Brad Thomas Aagaard. Finite-element simulations of earthquakes , 2000 .
[2] S. Day. Three-dimensional simulation of spontaneous rupture: The effect of nonuniform prestress , 1982, Bulletin of the Seismological Society of America.
[3] Marvin W. Halling,et al. Near-Source Ground Motion and its Effects on Flexible Buildings , 1995 .
[4] Ralph J. Archuleta,et al. The Three-Dimensional Dynamics of Dipping Faults , 2000 .
[5] D. Boore. Effect of Baseline Corrections on Displacements and Response Spectra for Several Recordings of the 1999 Chi-Chi, Taiwan, Earthquake , 2004 .
[6] Toru Ouchi,et al. The 1999 Chi-Chi (Taiwan) Earthquake: Earthquake Fault and Strong Motions , 2004 .
[7] C. R. Allen,et al. Evidence for Unusually Strong Near-field Ground Motion on the Hanging Wall of the San Fernando Fault during the 1971 Earthquake , 1998 .
[8] Kim B. Olsen,et al. Three-Dimensional Simulation of a Magnitude 7.75 Earthquake on the San Andreas Fault , 1995, Science.
[9] C. Ji,et al. Slip distribution and tectonic implication of the 1999 Chi‐Chi, Taiwan, Earthquake , 2001 .
[10] Thomas H. Heaton,et al. Dynamic Earthquake Ruptures in the Presence of Lithostatic Normal Stresses: Implications for Friction Models and Heat Production , 2001 .
[11] S. Day,et al. Fault Geometry and the Dynamics of the 1999 Chi-Chi (Taiwan) Earthquake , 2004 .
[12] Kim B. Olsen,et al. Three-dimensional simulation of earthquakes on the Los Angeles fault system , 1996, Bulletin of the Seismological Society of America.
[13] Tomohiro Inoue,et al. 3D simulation of near-field strong ground motion based on dynamic modeling , 1998, Bulletin of the Seismological Society of America.
[14] Shui-Beih Yu,et al. Spatial and Temporal Distribution of Slip for the 1999 Chi-Chi, Taiwan, Earthquake , 2004 .
[15] Chu-Chuan Peter Tsai,et al. Characteristics of strong ground motion across a thrust fault tip from the September 21, 1999, Chi‐Chi, Taiwan earthquake , 2000 .
[16] John F. Hall,et al. Parameter study of the response of moment-resisting steel frame buildings to near-source ground motions , 1995 .
[17] D. J. Andrews,et al. Rupture velocity of plane strain shear cracks , 1976 .
[18] Tzay-Chyn Shin,et al. CWB Free-Field Strong-Motion Data from the 21 September Chi-Chi, Taiwan, Earthquake , 2004 .
[19] Thomas H. Heaton,et al. Relationships between Peak Ground Acceleration, Peak Ground Velocity, and Modified Mercalli Intensity in California , 1999 .
[20] Kim B. Olsen,et al. Three-Dimensional Dynamic Simulation of the 1992 Landers Earthquake , 1997 .
[21] Ralph J. Archuleta,et al. Three-dimensional numerical simulations of dynamic faulting in a half-space , 1978, Bulletin of the Seismological Society of America.
[22] R. Madariaga,et al. Modeling Dynamic Rupture in a 3 D Earthquake Fault Model by , 1998 .
[23] R. Madariaga,et al. Modeling dynamic rupture in a 3D earthquake fault model , 1998, Bulletin of the Seismological Society of America.
[24] O. Ghattas,et al. Simulations of Long-Period Ground Motions during the 1995 Hyogoken-Nanbu ( Kobe ) Earthquake using 3 D Finite Element Method , 1998 .
[25] Robert W. Graves,et al. Three-dimensional finite-difference modeling of the San Andreas fault: Source parameterization and ground-motion levels , 1998, Bulletin of the Seismological Society of America.
[26] Kojiro Irikura,et al. Three-dimensional simulation of the near-fault ground motion for the 1995 Hyogo-Ken Nanbu (Kobe), Japan, earthquake , 1998, Bulletin of the Seismological Society of America.
[27] G. Beroza,et al. A spatial random field model to characterize complexity in earthquake slip , 2002 .
[28] N. A. Haskell. Elastic displacements in the near-field of a propagating fault , 1969 .
[29] Thomas H. Heaton,et al. Characterization of Near-Source Ground Motions with Earthquake Simulations , 2001 .
[30] Paul Segall,et al. Fault geometry and slip distribution of the 1999 Chi‐Chi, Taiwan Earthquake imaged from inversion of GPS data , 2001 .
[31] K. B. Olsen,et al. Constraints on Stress and Friction from Dynamic Rupture Models of the 1994 Northridge, California, Earthquake , 2000 .
[32] Ralph J. Archuleta,et al. Effects of fault finiteness on near-source ground motion , 1981 .
[33] John F. Hall,et al. Seismic response of steel frame buildings to near‐source ground motions , 1998 .
[34] T B Comstock,et al. U. S. Geological Survey , 1907, Radiocarbon.
[35] Kojiro Irikura,et al. Source model of the 1995 Hyogo-Ken Nanbu earthquake and simulation of near-source ground motion , 1998, Bulletin of the Seismological Society of America.
[36] D. Wells,et al. New empirical relationships among magnitude, rupture length, rupture width, rupture area, and surface displacement , 1994, Bulletin of the Seismological Society of America.
[37] T. Heaton. Evidence for and implications of self-healing pulses of slip in earthquake rupture , 1990 .
[38] J. Boatwright,et al. Correlation of Ground Motion and Intensity for the 17 January 1994 Northridge, California, Earthquake , 2001 .
[39] N. Abrahamson,et al. Modification of Empirical Strong Ground Motion Attenuation Relations to Include the Amplitude and Duration Effects of Rupture Directivity , 1997 .
[40] Chu-Chuan Peter Tsai,et al. An Observation of Rupture Pulses of the 20 September 1999 Chi-Chi, Taiwan, Earthquake from Near-Field Seismograms , 2004 .
[41] Jeen‐Hwa Wang,et al. Three-Dimensional Seismic Velocity Structure of the Crust and Uppermost Mantle beneath Taiwan , 1996 .
[42] Teh-Ru Alex Song,et al. Spatial slip distribution of the September 20, 1999, Chi‐Chi, Taiwan, Earthquake (MW7.6) —Inverted from teleseismic data , 2000 .