Estimation of the High-Frequency Radiation of the 2000 Tottori (Japan) Earthquake Based on a Dynamic Model of Fault Rupture: Application to the Strong Ground Motion Simulation

Abstract In the present study we investigate the high-frequency (HF) radiation mechanism of the 2000 Tottori earthquake in Japan based on a 3D spontaneous fault rupture dynamic model. We generalize the model of HF radiation of a suddenly stopping circular crack (Madariaga, 1977; Boatwright, 1982) to the radiation from a general 3D rupture in a planar fault, where HF is radiated during gradual changes of rupture velocity at the rupture front. Local rupture velocity changes are expressed as the divergence of local rupture velocity vectors that are derived from gradients of rupture times from the dynamic model. Our numerical model of the Tottori earthquake indicates that rupture velocity changes are largely induced by barriers (locally stronger fault sections) across the fault plane and that HF radiation mainly originates within asperities (large stress-drop regions) in areas where the product of dynamic stress drop and rupture velocity changes is maximum. We develop a strong ground motion simulation methodology that incorporates HF radiation inferred from a dynamic fault rupture model. Using this methodology we investigate the HF radiation of the Tottori earthquake by inverting observed near-source acceleration envelopes of the earthquake. Our inversion results corroborate that HF radiation originates within asperities and show that significant HF radiation represents no more than a 20% of the total asperity area. Our results show that the incorporation of a directivity factor, on the basis of a well-defined physical rupture model to the radiation pattern leads to a significant improvement in fitting of observed ground motions. Our simulated near-source strong ground motions of the Tottori earthquake are also able to reproduce the ω -2 radiation theoretically predicted in 2D dynamic fault rupture models.

[1]  Raul Madariaga,et al.  High-frequency radiation from crack (stress drop) models of earthquake faulting , 1977 .

[2]  M. Takeo,et al.  Determination of constitutive relations of fault slip based on seismic wave analysis , 1997 .

[3]  J. D. Riera,et al.  The Importance of the Dynamic Source Effects on Strong Ground Motion during the 1999 Chi-Chi, Taiwan, Earthquake: Brief Interpretation of the Damage Distribution on Buildings , 2004 .

[4]  G. Beroza,et al.  A hybrid method for calculating near-source, broadband seismograms: application to strong motion prediction , 2003 .

[5]  Breaking of a single asperity: Rupture process and seismic radiation , 1983 .

[6]  How Frictional Properties Lead to Either Rupture-Front Focusing or Cracklike Behavior , 2007 .

[7]  Takeshi Nishimura,et al.  Broadband Source Process of the 1998 Iwate Prefecture, Japan, Earthquake as Revealed from Inversion Analyses of Seismic Waveforms and Envelopes , 2002 .

[8]  Kojiro Irikura,et al.  Source Characterization for Broadband Ground-Motion Simulation: Kinematic Heterogeneous Source Model and Strong Motion Generation Area , 2003 .

[9]  Ralph J. Archuleta,et al.  Near‐source ground motion from steady state dynamic rupture pulses , 2005 .

[10]  J. Carlson,et al.  Distinguishing barriers and asperities in near-source ground motion , 2005 .

[11]  Kojiro Irikura,et al.  A technique for simulating strong ground motion using hybrid Green's function , 1998, Bulletin of the Seismological Society of America.

[12]  J. D. Riera,et al.  Distribution of Dynamic and Static Stress Changes during 2000 Tottori (Japan) Earthquake: Brief Interpretation of the Earthquake Sequences; Foreshocks, Mainshock and Aftershocks , 2002 .

[13]  K. Atakan,et al.  Sensitivity of Ground-Motion Simulations to Earthquake Source Parameters: A Case Study for Istanbul, Turkey , 2007 .

[14]  Hiroyuki Fujiwara,et al.  STRONG-MOTION SEISMOGRAPH NETWORK OPERATED BY NIED: K-NET AND KiK-net , 2004 .

[15]  Mitiyasu Ohnaka,et al.  A Physical Scaling Relation Between the Size of an Earthquake and its Nucleation Zone Size , 2000 .

[16]  K. Irikura,et al.  Estimation of strong ground motion in broad-frequency band based on a seismic source scaling model and an empirical Green's function technique , 1994 .

[17]  A. Herrero,et al.  A kinematic self-similar rupture process for earthquakes , 1994, Bulletin of the Seismological Society of America.

[18]  T. Satoh RADIATION PATTERN AND FMAX OF THE TOTTORI-KEN SEIBU EARTHQUAKE AND THE AFTERSHOCKS INFERRED FROM KIK-NET STRONG MOTION RECORDS , 2002 .

[19]  Steven M. Day,et al.  Stochastic Fault Stress: Implications for Fault Dynamics and Ground Motion , 2002 .

[20]  Generation of New Cracks Accompanied by the Dynamic Shear Rupture Propagation of the 2000 Tottori (Japan) Earthquake , 2003 .

[21]  Near-fault strong motion complexity of the 2000 Tottori earthquake (Japan) from a broadband source asperity model , 2004 .

[22]  High-frequency radiation process during earthquake faulting—envelope inversion of acceleration seismograms from the 1993 Hokkaido-Nansei-Oki, Japan, earthquake , 1997, Bulletin of the Seismological Society of America.

[24]  Pengcheng Liu,et al.  Calculation of Broadband Time Histories of Ground Motion, Part II: Kinematic and Dynamic Modeling Using Theoretical Green’s Functions and Comparison with the 1994 Northridge Earthquake , 2005 .

[25]  Y. Hisada A Theoretical Omega-Square Model Considering Spatial Variation in Slip and Rupture Velocity. Part 2: Case for a Two-Dimensional Source Model , 2001 .

[26]  L. Neil Frazer,et al.  Use of ray theory to calculate high-frequency radiation from earthquake sources having spatially variable rupture velocity and stress drop , 1984 .

[27]  David M. Boore,et al.  Average body-wave radiation coefficients , 1984 .

[28]  Luis A. Dalguer,et al.  Staggered-grid split-node method for spontaneous rupture simulation , 2007 .

[29]  Gregory C. Beroza,et al.  A Pseudo-Dynamic Approximation to Dynamic Rupture Models for Strong Ground Motion Prediction , 2004 .

[30]  S. Day Three-dimensional simulation of spontaneous rupture: The effect of nonuniform prestress , 1982, Bulletin of the Seismological Society of America.

[31]  M. Bouchon,et al.  Heterogeneous distribution of the dynamic source parameters of the 1999 Chi-Chi, Taiwan, earthquake , 2003 .

[32]  Pengcheng Liu,et al.  Prediction of Broadband Ground-Motion Time Histories: Hybrid Low/High- Frequency Method with Correlated Random Source Parameters , 2006 .

[33]  J. Rice Heating and weakening of faults during earthquake slip , 2006 .

[34]  P. Spudich,et al.  Earthquake fracture energy inferred from kinematic rupture models on extended faults , 2005 .

[35]  Kojiro Irikura,et al.  Surface Rupturing and Buried Dynamic-Rupture Models Calibrated with Statistical Observations of Past Earthquakes , 2008 .

[36]  K. Atakan,et al.  Simulated Strong Ground Motions for the Great M 9.3 Sumatra-Andaman Earthquake of 26 December 2004 , 2007 .

[37]  Thorne Lay,et al.  Quantitative Seismology, Second Edition , 2003 .

[38]  Kuvvet Atakan,et al.  Strong ground motion estimation in the Sea of Marmara region (Turkey) based on a scenario earthquake , 2004 .

[39]  F. Waldhauser,et al.  Detailed Fault Structure of the 2000 Western Tottori, Japan, Earthquake Sequence , 2003 .

[40]  Tetsuo Kubo,et al.  Near-fault strong motion complexity of the 2000 Tottori earthquake (Japan) from a broadband source asperity model , 2004 .

[41]  R. Madariaga,et al.  Dynamic Propagation and Interaction of a Rupture Front on a Planar Fault , 2000 .

[42]  M. Ohtake,et al.  Seismogram envelope inversion for the spatial distribution of high‐frequency energy radiation from the earthquake fault: Application to the 1994 far east off Sanriku earthquake, Japan , 1998 .

[43]  Kojiro Irikura,et al.  Simulation of Near-Fault Strong-Ground Motion Using Hybrid Green's Functions , 2000 .

[44]  Y. Yagi,et al.  Stress-Breakdown Time and Slip-Weakening Distance Inferred from Slip-Velocity Functions on Earthquake Faults , 2003 .

[45]  Shawn Larsen,et al.  Calculation of broadband time histories of ground motion: Comparison of methods and validation using strong-ground motion from the 1994 Northridge earthquake , 1999, Bulletin of the Seismological Society of America.

[46]  S. Day,et al.  Comparison of finite difference and boundary integral solutions to three‐dimensional spontaneous rupture , 2005 .

[47]  John Boatwright A dynamic model for far-field acceleration , 1982 .

[48]  E. Dunham,et al.  A Supershear Transition Mechanism for Cracks , 2003, Science.

[49]  Yoshiaki Hisada,et al.  A Theoretical Omega-Square Model Considering the Spatial Variation in Slip and Rupture Velocity , 2000 .

[50]  Massimo Cocco,et al.  The envelopes of acceleration time histories , 1993 .

[51]  N. Abrahamson,et al.  Characterizing Crustal Earthquake Slip Models for the Prediction of Strong Ground Motion , 1999 .

[52]  K. Irikura,et al.  Estimation of dynamic rupture parameters from the radiated seismic energy and apparent stress , 2000 .

[53]  Yuehua Zeng,et al.  A composite source model of the 1994 Northridge earthquake using genetic algorithms , 1996, Bulletin of the Seismological Society of America.

[54]  Walter H. F. Smith,et al.  New, improved version of generic mapping tools released , 1998 .

[55]  Keiiti Aki,et al.  Mapping of the high-frequency source radiation for the Loma Prieta Earthquake, California , 1993 .

[56]  Mitiyasu Ohnaka,et al.  A constitutive scaling law and a unified comprehension for frictional slip failure, shear fracture of intact rock, and earthquake rupture , 2003 .

[57]  Gregory C. Beroza,et al.  Strong Ground-Motion Prediction from Stochastic-Dynamic Source Models , 2003 .

[58]  Estimation of High-frequency Wave Radiation Areas on the Fault Plane of the 1995 Hyogo-ken Nanbu Earthquake by the Envelope Inversion of Acceleration Seismograms , 1996 .

[59]  N. Kame,et al.  Seismic radiation from dynamic coalescence, and the reconstruction of dynamic source parameters on a planar fault , 2008 .

[60]  Tamao Sato,et al.  Seismic radiation from circular cracks growing at variable rupture velocity , 1994, Bulletin of the Seismological Society of America.

[61]  David M. Boore,et al.  Simulation of Ground Motion Using the Stochastic Method , 2003 .

[62]  J. Achenbach,et al.  Ray method for elastodynamic radiation from a slip zone of arbitrary shape , 1978 .

[63]  D. J. Andrews,et al.  Rupture velocity of plane strain shear cracks , 1976 .

[64]  K. Olsen,et al.  On the Effects of Non-planar Geometry for Blind Thrust Faults on Strong Ground Motion , 2004 .

[65]  P. M. Mai,et al.  Bayesian inference of kinematic earthquake rupture parameters through fitting of strong motion data , 2008 .

[66]  Kuvvet Atakan,et al.  Strong ground motion estimation in the Marmara Sea region (Turkey) based on a scenario earthquake , 2004 .

[67]  Yoshiaki Ida,et al.  Cohesive force across the tip of a longitudinal‐shear crack and Griffith's specific surface energy , 1972 .

[68]  K. Irikura,et al.  Estimation of high-frequency wave radiation areas on the fault plane by the envelope inversion of acceleration seismograms , 1996 .