Nonlinear Processes in Geophysics www.nonlin-processes-geophys.net 1023-5809 1607-7946 3 1 1996 10.5194/npg-3-1-1996 http://www.nonlin-processes-geophys.net/3/1/1996/ http://www.nonlin-processes-geophys.net/3/1/1996/npg-3-1-1996.html http://www.nonlin-processes-geophys.net/3/1/1996/npg-3-1-1996.pdf 1 12 0000-00-00 Faults self-organized by repeated earthquakes in a quasi-static antiplane crack model D. Sornette C. Vanneste Laboratoire de Physique de la Matière Condensée, CNRS URA 190, Université de Nice-Sophia Antipolis, B.P. 71, Parc Valrose, 06108 Nice Cedex 2, France We study a 2D quasi-static discrete crack anti-plane model of a tectonic plate with long range elastic forces and quenched disorder. The plate is driven at its border and the load is transferred to all elements through elastic forces. This model can be considered as belonging to the class of self-organized models which may exhibit spontaneous criticality, with four additional ingredients compared to sandpile models, namely quenched disorder, boundary driving, long range forces and fast time crack rules. In this "crack" model, as in the "dislocation" version previously studied, we find that the occurrence of repeated earthquakes organizes the activity on well-defined fault-like structures. In contrast with the "dislocation" model, after a transient, the time evolution becomes periodic with run-aways ending each cycle. This stems from the "crack" stress transfer rule preventing criticality to organize in favour of cyclic behaviour. For sufficiently large disorder and weak stress drop, these large events are preceded by a complex spacetime history of foreshock activity, characterized by a Gutenberg-Richter power law distribution with universal exponent <i> B<b> </b></i> = 1&#177;0.05. This is similar to a power law distribution of small nucleating droplets before the nucleation of the macroscopic phase in a first-order phase transition. For large disorder and large stress drop, and for certain specific initial disorder configurations, the stress field becomes frustrated in fast time: out-of-plane deformations (thrust and normal faulting) and/or a genuine dynamics must be introduced to resolve this frustration.