Constraints on stress and friction from dynamic rupture models of the 1994Northridge, California, earthquake

Citation
Sb. Nielsen et Kb. Olsen, Constraints on stress and friction from dynamic rupture models of the 1994Northridge, California, earthquake, PUR A GEOPH, 157(11-12), 2000, pp. 2029-2046
Citations number
22
Categorie Soggetti
Earth Sciences
Journal title
PURE AND APPLIED GEOPHYSICS
ISSN journal
00334553 → ACNP
Volume
157
Issue
11-12
Year of publication
2000
Pages
2029 - 2046
Database
ISI
SICI code
0033-4553(200012)157:11-12<2029:COSAFF>2.0.ZU;2-4
Abstract
We have simulated several scenarios of dynamic rupture propagation for the 1994 Northridge, California, earthquake, using a three-dimensional finite-d ifference method. The simulations use a rate- and slip-weakening friction l aw, starting from a range of initial conditions of stress and frictional pa rameters. A critical balance between initial conditions and friction parame ters must be met in order to obtain a moment as well as a final slip distri bution in agreement with kinematic slip inversion results. We find that the rupture process is strongly controlled by the average stress and connectiv ity of high-stress patches on the fault. In particular, a strong connectivi ty of the high-stress patches is required in order to promote the rupture p ropagation from the initial nucleation to the remaining part of the Fault. Moreover, we find that a small amount of rate-weakening is needed in order to obtain a level of inhomogeneity in the final slip, similar to that obtai ned in the kinematic inversion results. However, when the amount of rate-we akening is increased, the overall moment drops dramatically unless the aver age prestress is raised to unrealistic levels. A velocity-weakening paramet er on the order of 10 cm per second is found to be adequate for an average prestress of about a hundred bars. The presence of the free surface and of the uppermost low-impedance layers in the model are found to have negligibl e influence on the rupture dynamics itself, because the top of the fault is at a depth of several kilometers. The 0.1-0.5 Hz radiated waves from the d ynamic simulation provides a good fit to strong motion data at sites NWH an d SSA. Underprediction of the recorded peak amplitude at JFP is likely due to omission of near-surface low velocity and 3-D basin effects in the simul ations.