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Annual Meeting - SCEC.org

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Group 1 – CSEP | Poster Abstracts<br />

relative shear displacement of each fault node. The fault nodes are tested for contact with the<br />

opposite fault member at each time step. This DEM model does not suffer from numerical<br />

instability when discontinuities occur (e.g., instantaneous friction changes, fault separation, etc.).<br />

Thus arbitrary friction laws and fault surface roughness' can be incorporated.<br />

A smooth fault is used to emulate AEA08; the DEM model incorporates the AEA08 material<br />

properties and surface topography. The initial stress state is obtained by displacing the nodal<br />

positions and cycling the damped model to quiescence. Initial investigations used linear time<br />

weakening friction following AEA08. The DEM model produces ground motions for the maximum<br />

slip event at the repository location which are very similar to AEA08 motions. An instantaneous<br />

friction law which drops from static to dynamic value in one time step very slightly increases the<br />

rupture velocity and yields nearly identical ground motions. Fault separation occurs locally near<br />

the free surface for very short time periods. AEA08 results for the “smooth” supershear and<br />

subshear 2.7 m slip cases compare favorably with the DEM ground motions with and without time<br />

weakening. These results indicate that beyond modulating the rupture velocity, frictional<br />

weakening is not a necessary component of dynamic rupture simulations utilizing DEM. These<br />

results strongly suggest that the physical significance of the so-called critical slip weakening<br />

distance must be scrutinized.<br />

1-071<br />

OBSERVED RELATIONS AMONG FAULT STRENGTH LOSS, STRESS DROP, SLIP<br />

VELOCITY, AND NEAR-FAULT PARTICLE VELOCITY DURING DYNAMIC<br />

RUPTURE PROPAGATION, AND THEIR IMPLICATIONS FOR LIMITS ON GROUND<br />

MOTION Beeler N, Kilgore BD, Boettcher M, McGarr A, Fletcher J, Evans J, and Baker S<br />

Extreme ground motions implied by the PSHA at Yucca Mountain at low exceedance probability<br />

require earthquake stress drop to approach the in situ shear stress. Lab rupture propagation<br />

experiments and seismic studies are not generally consistent with this requirement; static stress<br />

drops are

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