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Earthquake source characteristics from dynamic rupture with constrained stochastic fault stress
Author(s) -
Ripperger J.,
Ampuero J.P.,
Mai P. M.,
Giardini D.
Publication year - 2007
Publication title -
journal of geophysical research: solid earth
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/2006jb004515
Subject(s) - earthquake rupture , slip (aerodynamics) , stress field , geology , stress (linguistics) , nucleation , fault plane , statistical physics , stochastic process , moment (physics) , stochastic modelling , mechanics , fault (geology) , seismology , mathematics , physics , classical mechanics , structural engineering , engineering , statistics , linguistics , philosophy , finite element method , thermodynamics
One of the challenging tasks in predicting near‐source ground motion for future earthquakes is to anticipate the spatiotemporal evolution of the rupture process. The final size of an event but also its temporal properties (propagation velocity, slip velocity) depend on the distribution of shear stress on the fault plane. Though these incipient stresses are not known for future earthquakes, they might be sufficiently well characterized in a stochastic sense. We examine the evolution of dynamic rupture in numerical models of a fault subjected to heterogeneous stress fields with varying statistical properties. By exploring the parameter space of the stochastic stress characterization for a large number of random realizations we relate generalized properties of the resulting events to the stochastic stress parameters. The nucleation zone of the simulated earthquake ruptures in general has a complex shape, but its average size is found to be independent of the stress field parameterization and is determined only by the material parameters and the friction law. Furthermore, we observe a sharp transition in event size from small to system‐wide events, governed mainly by the standard deviation of the stress field. A simplified model based on fracture mechanics is able to explain this transition. Finally, we find that the macroscopic rupture parameters (e.g., moment, moment rate, seismic energy) of our catalog of model quakes are generally consistent with observational data.

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