The influence of the source on the high-frequency behavior of the near-Field acceleration spectrum: A numerical study

The hypothesis that particular physical properties of the earth at the source can affect the radiation of high-frequency waves was numerically investigated. Two factors have been considered: a non-elastic behavior of the material at the crack tip (i.e presence of a cohesive zone) and the kinematics of the rupture front. Using the discrete wave number method, we calculated complete near-source synthetic spectra radiated by a circular shear crack model. The two processes can explain an exponential decrease of the acceleration spectrum at high frequencies. Moreover, they can be differentiated. In the case of a final smooth deceleration of the rupture front, the rate of decay of the acceleration spectra is equivalent in all the azimuths. A clear azimuthal dependence exists in the presence of a cohesive zone, with the maximum rate of decay being observed in the direction of the fault strike. The parameter fmax varies as the ratio of the rupture velocity over the length of the cohesive zone for the non-elastic model and as the inverse of the duration of the deceleration of the rupture front when the rupture front stops smoothly. These two models result in a decay of spectral amplitude at high frequency that mimics the effect of the anelastic attenuation.

[1]  Michel Campillo,et al.  A theoretical study of the radiation from small strikeslip earthquakes at close distances , 1983 .

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

[3]  M. Bouchon A simple method to calculate Green's functions for elastic layered media , 1981 .

[4]  K. Aki Characterization of barriers on an earthquake fault , 1979 .

[5]  Mitiyasu Ohnaka,et al.  Constitutive relations between dynamic physical parameters near a tip of the propagating slip zone during stick-slip shear failure , 1987 .

[6]  B. V. Kostrov,et al.  Selfsimilar problems of propagation of shear cracks , 1964 .

[7]  Apostolos S. Papageorgiou,et al.  On two characteristic frequencies of acceleration spectra: Patch corner frequency and fmax , 1988 .

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

[9]  John G. Anderson,et al.  A MODEL FOR THE SHAPE OF THE FOURIER AMPLITUDE SPECTRUM OF ACCELERATION AT HIGH FREQUENCIES , 1984 .

[10]  R. Madariaga Dynamics of an expanding circular fault , 1976, Bulletin of the Seismological Society of America.

[11]  G. I. Barenblatt The formation of equilibrium cracks during brittle fracture. General ideas and hypotheses. Axially-symmetric cracks , 1959 .

[12]  M. Campillo Numerical evaluation of near-field, high-frequency radiation from quasi-dynamic circular faults , 1983 .

[13]  A. Papageorgiou,et al.  A specific barrier model for the quantitative description of inhomogeneous faulting and the prediction of strong ground motion. I. Description of the model , 1983 .

[14]  K. Aki,et al.  Seismic source time function of propagating longitudinal‐shear cracks , 1972 .