Calculation of broadband time histories of ground motion: Comparison of methods and validation using strong-ground motion from the 1994 Northridge earthquake

Citation
S. Hartzell et al., Calculation of broadband time histories of ground motion: Comparison of methods and validation using strong-ground motion from the 1994 Northridge earthquake, B SEIS S AM, 89(6), 1999, pp. 1484-1504
Citations number
92
Categorie Soggetti
Earth Sciences
Journal title
BULLETIN OF THE SEISMOLOGICAL SOCIETY OF AMERICA
ISSN journal
00371106 → ACNP
Volume
89
Issue
6
Year of publication
1999
Pages
1484 - 1504
Database
ISI
SICI code
0037-1106(199912)89:6<1484:COBTHO>2.0.ZU;2-K
Abstract
This article compares techniques for calculating broadband time histories o f ground motion in the near field of a finite fault by comparing synthetics with the strong-motion data set for the 1994 Northridge earthquake. Based on this comparison, a preferred methodology is presented. Ground-motion-sim ulation techniques are divided into two general methods: kinematic- and com posite-fault models. Green's functions of three types are evaluated: stocha stic, empirical, and theoretical. A hybrid scheme is found to give the best fit to the Northridge data. Low frequencies (< 1 Hz) are calculated using a kinematic-fault model and a 3D finite-difference code to propagate energy through a realistic 3D velocity structure. High frequencies (> 1 Hz) are c alculated using a composite-fault model with a fractal subevent size distri bution and stochastic, bandlimited, white-noise Green's functions, At frequ encies below 1 Hz, theoretical elastic-wave-propagation synthetics introduc e proper seismic-phase arrivals of body waves and surface waves. The 3D vel ocity structure more accurately reproduces record durations for the deep se dimentary basin structures found in the Los Angeles region. At frequencies above I Hz, scattering effects become important and wave propagation is mor e accurately represented by stochastic Green's functions. A fractal subeven t size distribution for the composite fault model ensures an omega(-2) spec tral shape over the entire frequency band considered (0.1-20 Hz).