A Generalization of the Double-Corner-Frequency Source Spectral Model and Its Use in the SCEC BBP Validation Exercise

The stochastic method of simulating ground motions requires the speci- fication of the shape and scaling with magnitude of the source spectrum. The spectral models commonly used are either single-corner-frequency or double-corner- frequency models, but the latter have no flexibility to vary the high-frequency spectral levels for a specified seismic moment. Two generalized double-corner-frequency ω 2 source spectral models are introduced, one in which two spectra are multiplied to- gether and another where they are added. Both models have a low-frequency depend- ence controlled by the seismic moment and a high-frequency spectral level controlled by the seismic moment and a stress parameter. Awide range of spectral shapes can be obtained from these generalized spectral models, which makes them suitable for in- versions of data to obtain spectral models that can be used in ground-motion simu- lations in situations in which adequate data are not available for purely empirical determinations of ground motions, such as in stable continental regions. As an exam- ple of the use of the generalized source spectral models, data from up to 40 stations from seven events, plus response spectra at two distances and two magnitudes from recent ground-motion prediction equations, were inverted to obtain the parameters controlling the spectral shapes, as well as a finite-fault factor that is used in point- source, stochastic-method simulations of ground motion. The fits to the data are com- parable to or even better than those from finite-fault simulations, even for sites close to large earthquakes.

[1]  Thu T. Duong,et al.  Author Correction: An Autogenously Regulated Expression System for Gene Therapeutic Ocular Applications , 2018, Scientific Reports.

[2]  Annemarie S. Baltay,et al.  Understanding the Magnitude Dependence of PGA and PGV in NGA‐West 2 Data , 2014 .

[3]  D. Boore What Do Data Used to Develop Ground-Motion Prediction Equations Tell Us About Motions Near Faults? , 2014, Pure and Applied Geophysics.

[4]  Timothy D. Ancheta,et al.  NGA-West2 Research Project , 2014 .

[5]  G. Atkinson,et al.  Equivalent Point‐Source Modeling of Moderate‐to‐Large Magnitude Earthquakes and Associated Ground‐Motion Saturation Effects , 2014 .

[6]  D. Boore The Uses and Limitations of the Square‐Root‐Impedance Method for Computing Site Amplification , 2013 .

[7]  Shahram Pezeshk,et al.  Hybrid Empirical Ground-Motion Prediction Equations for Eastern North America Using NGA Models and Updated Seismological Parameters , 2011 .

[8]  D. Boore Comparing Stochastic Point-Source and Finite-Source Ground-Motion Simulations: SMSIM and EXSIM , 2009 .

[9]  I. M. Idriss,et al.  Comparisons of the NGA Ground-Motion Relations , 2008 .

[10]  Gail M. Atkinson,et al.  Empirical Ground-Motion Relations for Subduction-Zone Earthquakes and Their Application to Cascadia and Other Regions , 2003 .

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

[12]  W. Silva,et al.  Stochastic Modeling of California Ground Motions , 2000 .

[13]  Luca Malagnini,et al.  Attenuation and excitation of three-component ground motion in southern California , 1999 .

[14]  David M. Boore,et al.  Site amplifications for generic rock sites , 1997, Bulletin of the Seismological Society of America.

[15]  R. Haddon,et al.  Earthquake source spectra in eastern North America , 1996, Bulletin of the Seismological Society of America.

[16]  G. Atkinson,et al.  Ground-motion relations for eastern North America , 1995, Bulletin of the Seismological Society of America.

[17]  L. M. Baker,et al.  Attenuation near Anza, California , 1988 .

[18]  David M. Boore,et al.  Short-period P- and S-wave radiation from large earthquakes: Implications for spectral scaling relations , 1986 .

[19]  W. B. Joyner,et al.  A scaling law for the spectra of large earthquakes , 1984 .

[20]  D. Boore Stochastic simulation of high-frequency ground motions based on seismological models of the radiated spectra , 1983 .

[21]  Robin K. McGuire,et al.  The character of high-frequency strong ground motion , 1981 .

[22]  H. Kanamori,et al.  A moment magnitude scale , 1979 .

[23]  J. Brune Tectonic stress and the spectra of seismic shear waves from earthquakes , 1970 .

[24]  G. Toro MODIFICATION OF THE TORO ET AL. (1997) ATTENUATION EQUATIONS FOR LARGE MAGNITUDES AND SHORT DISTANCES , 2002 .

[25]  David M. Boore,et al.  SMSIM — Fortran Programs for Simulating Ground Motions from Earthquakes: Version 2.3 — A Revision of OFR 96–80–A , 2000 .