Annual Meeting - SCEC.org
Annual Meeting - SCEC.org
Annual Meeting - SCEC.org
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Group 2 – FARM | Poster Abstracts<br />
Previous studies incorporated plastic yielding in simulations of dynamic rupture (Andrews, 1975,<br />
2005; Ben-Zion and Shi, 2005; Templeton et al., 2008) while keeping the elastic moduli unchanged.<br />
In this work we examine the dynamics of earthquake ruptures and generated motion in a model<br />
consisting of a frictional fault in a medium governed by a continuum damage rheology for the<br />
evolution of elastic moduli (e.g. Lyakhovsky and Ben-Zion, 2008). We perform numerical<br />
simulations based on the Spectral Element Method to study how the parameters of the friction law,<br />
damage rheology and background stress control the rate of growth of the off-fault damage zone,<br />
the steady-state rupture speed, the energy balance, and the maximum slip rate and ground motion.<br />
We find that, the maximum slip velocity, steady-state rupture speed and peak ground motion with<br />
increasing values of the constitutive parameters Cd (the inverse of a damage timescale) and Cv (the<br />
intensity of damage related plasticity). The relation between Cv, Cd and the rate of off-fault<br />
damage growth with rupture distance is less trivial: the damage-induced bimaterial contrast grows<br />
faster with increasing Cd, and the sign of the contrast changes at low Cv. We also compare peak<br />
ground motion in our damage model to analogous simulations using Coulomb plastic yielding.<br />
2-079<br />
RUPTURE PROPAGATION AND SLIP PARTITIONING ON AN OBLIQUE UPWARD-<br />
BRANCHING FAULT SYSTEM Oglesby DD, Bowman D, and Nunley ME<br />
We use dynamic 3-D finite element analysis to investigate slip partitioning and rupture<br />
propagation on an oblique left-lateral/normal fault system that branches near the surface into<br />
vertical and non-vertical branches. The model consists of a 70° dipping oblique-slip fault that<br />
extends from a depth of 15km to 5km depth and then branches upwards into a vertical segment<br />
and a segment dipping 45° The use of a simple regional stress field resolved onto all fault segments<br />
results in rupture propagation only on the base and vertical faults. However, the addition of a 2km<br />
by 3km barrier onto the bottom portion of the vertical fault causes enough of a stress perturbation<br />
on the upper dipping fault to nucleate rupture on this segment, resulting in a strongly partitioned<br />
slip distribution in the system. In all cases, strike-slip motion is concentrated on the vertical fault,<br />
and dip-slip motion is concentrated on the dipping fault. These results are not sensitive to the size<br />
and along-strike location of the barrier. Other observations in our models show that as the dipping<br />
fault slips, it induces a small amount of backwards slip on the vertical fault due to the high stress<br />
drop in our models, and the close proximity of the two branch segments. Our results may have<br />
important implications for the dynamics of branched faults and geometrically complex fault<br />
systems in general.<br />
2-080<br />
LABORATORY INVESTIGATIONS OF THE ORIGIN OF PULVERIZED ROCKS Yuan<br />
F, and Prakash V<br />
Zones of pulverized rock have been observed in surface outcrops adjacent to the fault cores of the<br />
San Andreas and other major faults in Southern California. These pulverized rocks consists of<br />
highly fractured fragments that still fit together and essentially preserve the original rock texture.<br />
The origin of these pulverized rocks is not clear, but their structural context indicates that they are<br />
clearly associated with faulting; an understanding of their origin might allow inferences to be<br />
drawn about the nature of dynamic slip on faults, including inferences concerning the coseismic<br />
resistance to slip, energy balance of earthquakes, and implications for ground motions and<br />
radiation patterns near faults. In the present study, a series of laboratory experiments are<br />
conducted on Westerly granite rock samples to investigate whether pulverized rocks can be<br />
produced under stress-wave loading conditions in the laboratory and whether they are diagnostic<br />
of any particular process of formation. In the first series of experiments a Split Hopkinson pressure<br />
2008 <strong>SCEC</strong> <strong>Annual</strong> <strong>Meeting</strong> | 183