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Annual Meeting - SCEC.org

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Poster Abstracts<br />

InSAR results based on C-band ERS data (Cakir et al., 2005) that suggested that the NAF segment near Ismetpasa may be only<br />

partially locked. If so, the deeper locked portion of the fault must be characterized by a higher stressing rate, and presumably<br />

shorter recurrence interval. We are modeling available InSAR and GPS data using numerical simulations of spontaneous<br />

earthquake sequences that incorporate laboratory-derived rate-and-state friction laws. The goal of these simulations is to<br />

constrain key parameters of fault friction such as the depth extent of the velocity-strengthening and velocity-weakening layers,<br />

the long-term fault slip rate, and stress evolution in the seismogenic crust.<br />

VARIABILITY OF SEISMIC SOURCE SPECTRA DERIVED FROM COHESIVE-ZONE MODELS OF A<br />

CIRCULAR RUPTURE PROPAGATING AT A CONSTANT SPEED (A-085)<br />

Y. Kaneko and P.M. Shearer<br />

Static stress drop of earthquakes is often estimated from far-field body-wave spectra using measurements of corner<br />

frequencies, together with seismic moment, which can be computed from the low-frequency part of the spectrum. Corner<br />

frequencies are used to infer the source dimension based on a specific theoretical model. The most widely used model is from<br />

Madariaga (1976), which considered a bilateral rupture expanding at a constant speed on a circular fault. This model assumes<br />

that the rupture front is characterized by an abrupt change of fault strength from a uniform initial prestress to a kinetic<br />

frictional stress, and hence the stress is singular at the rupture front. In this study, we investigate variability of source spectra<br />

derived from dynamic models of expanding bilateral ruptures on a circular fault with a cohesive zone that prevents a stress<br />

singularity at the rupture front. We study the dependence of far-field body-wave spectra on the rate of frictional weakening<br />

(which controls the cohesive zone size), rupture speed, and dynamic stress drop. For each source model, we compute far-field<br />

body-wave displacement synthetics for a homogeneous elastic space using the representation theorem (Aki and Richards,<br />

2002). Our results show that P- and S-wave corner frequencies of displacement spectra are systematically larger than those<br />

predicted by Madariaga (1976) and generally depend on the rate of frictional weakening in the source model, which affects the<br />

fracture-energy-density distribution on the fault. For a given rupture speed, the average of corner frequencies over the focal<br />

sphere is larger for source models with larger fracture energy. For ruptures propagating at 90 percent of the S-wave speed,<br />

the azimuthal average of P-wave corner frequencies in the case with the smallest fracture energy is about 20 percent larger<br />

than that of Madariaga (1976), which corresponds to about a factor of two difference in the inferred stress drop. Thus for these<br />

ruptures, application of the Madariaga model overestimates stress drops by factors of two or more, depending upon the<br />

fracture energy. We also find that the takeoff angle dependence of the corner frequencies for supershear ruptures is<br />

systematically different from that for subshear ruptures due to the difference in radiated wave fields for supershear and<br />

subshear ruptures.<br />

THREE DIMENSIONAL ELASTIC RESPONSE OF COMPLIANT FAULT ZONES TO NEARBY<br />

EARTHQUAKES: A THEORETIC STUDY (A-110)<br />

J. Kang and B. Duan<br />

Compliant fault zones have been detected along active faults by seismic<br />

investigations (trapped waves and travel time analysis) and InSAR observations. However, the width and depth extent of<br />

compliant fault zones are still under debate in the community. Numerical models of dynamic rupture build a bridge between<br />

theories and the geological and geophysical observations. Theoretical 2D plane-strain studies of elastic and inelastic response<br />

of compliant fault zones to nearby earthquake have been conducted by Duan [2010] and Duan et al [2010]. In this study, we<br />

further extend the experiments to 3D with a focus on elastic response. We are specifically interested in how residual<br />

displacements depend on the structure and properties of complaint fault zones, in particular on the width and depth extent.<br />

We conduct numerical experiments on various types of fault-zone models, including fault zones with a constant width along<br />

depth, with decreasing widths along depth, and with Hanning taper profiles of velocity reduction. . Our preliminary results<br />

suggest 1) the width of anomalous horizontal residual displacement is only indicative of the width of a fault zone near the<br />

surface, and 2) the vertical residual displacement contains information of the depth extent of compliant fault zones.<br />

A UNIFIED FINITE ELEMENT METHOD FOR HETEROGENEOUS ELASTIC MEDIA WITH LOW TO HIGH<br />

RATIO OF P- TO S-WAVE VELOCITIES (A-040)<br />

H. Karaoglu and J. Bielak<br />

This study reports on a mixed finite element formulation that overcomes certain limitations faced by low-order primal-based<br />

formulations. A primal-based formulation with displacement as the variable is a widely used method to solve wave-<br />

2011 <strong>SCEC</strong> <strong>Annual</strong> <strong>Meeting</strong> | 185

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