1980
DOI: 10.1029/jb085ib07p03867
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A stochastic fault model: 1. Static case

Abstract: The number‐size distribution of earthquakes requires that irregularities exist on a fault at all length scales. The assumption of self‐similar irregularity is used to formulate a stochastic description of the faulting process. A random irregularity is termed self similar if it remains statistically similar upon a change of length scale. Self‐similar geometric irregularity of a fault surface is represented in this model by stress and friction functions that fluctuate self similarly on a plane. If the set of rup… Show more

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Cited by 282 publications
(201 citation statements)
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“…While the role of fixed heterogeneities related to fault structure and properties versus heterogeneity arising solely from the nonlinear dynamics of rupture propagation is a source of active controversy, it is becoming apparent that both factors are present and contribute significantly to observed variations in coseismic slip (Shaw, 2004). The important implication of this rich field of studies is that (a) whatever the mechanism, the final slip distribution of a rupture can be characterized as being self-affine (Andrews, 1980); and (b) this slip distribution, though deterministic and causal, is difficult to predict.…”
Section: Earthquake Physicsmentioning
confidence: 99%
“…While the role of fixed heterogeneities related to fault structure and properties versus heterogeneity arising solely from the nonlinear dynamics of rupture propagation is a source of active controversy, it is becoming apparent that both factors are present and contribute significantly to observed variations in coseismic slip (Shaw, 2004). The important implication of this rich field of studies is that (a) whatever the mechanism, the final slip distribution of a rupture can be characterized as being self-affine (Andrews, 1980); and (b) this slip distribution, though deterministic and causal, is difficult to predict.…”
Section: Earthquake Physicsmentioning
confidence: 99%
“…[9] We compute the static shear-stress change from the refined coseismic slip model using a fast Fourier transform (FFT) method [Andrews, 1980;Ripperger and Mai, 2004], chosen because of its computational efficiency that allows the exploration of multiple model parameters. The 20 km × 20 km gridded slip model is initially downsampled via bicubic interpolation to a 1 km × 1 km grid, which serves as the input for the stress-change calculation.…”
Section: Minimum Stress Drop From the 27 February 2010 Maule Earthquakementioning
confidence: 99%
“…It is well known that the powerlaw moment-frequency scaling implied by the GR relation indicates that the earthquake rupture process is scale invariant (Andrews, 1980;Rundle, 1989). Thus, it follows that deviations from the GR relation, which are expected, by Correspondence to: M. H. Heimpel (mheimpel@phys.ualberta.ca) physical and geometrical constraints, at both small and large ends of earthquake size-frequency distributions, indicate the effect of characteristic scales of the fault or fault system.…”
Section: Introductionmentioning
confidence: 99%