Abstract

<p>The linear slip–weakening (SW) law, predicting that the traction decreases for increasing fault slip, is one of the most widely adopted governing models to describe the traction evolution and the stress release processes occurring during coseismic slip failures. We will show that, contrary to other constitutive models, the SW law inherently poses the problem of considering the Euclidean norm of the slip vector or its cumulative value along its path. In other words, it has the intrinsic problem of its analytical formulation, which does not have a solution a priori. By considering a fully dynamic, spontaneous, 3–D rupture problem, with rake rotation allowed, in this paper we explore whether these two formulations can lead to different results. We prove that, for homogeneous configurations, the two formulations give the same results, with a normalized difference less than 1%, which is comparable to the numerical error due to grid dispersion. In particular, we show that the total slip, the resulting seismic moment, the fracture energy density, the slip–weakening curve and the energy flux at the rupture front are practically identical in the two formulations. These findings contribute to reconcile the results presented in previous papers, where the two formulations have been differently employed. However, this coincidence is not the rule. Indeed, by considering models with a highly heterogeneous initial shear stress distribution, where the rake variation is significant, we have also demonstrated that the overall rupture history is quite different by assuming the two formulations, as well as the fault striations, the traction evolution and the scalar seismic moment. In this case the choice of the analytical formulation of the governing law does really matter.</p>

Highlights

  • It is well known that numerical experiments represent, in addition to theory and to laboratory experiments, a suitable way to explore natural phenomena

  • SW distance, the two formulations (1) and (2) produce practically the same results. This is basically due to the fact that the rake rotation is not so pronounced to induce variations in the computation of the frictional resistance specified by the linear SW law

  • The obvious problem is : what happens if the rake rotation is significant? In order to answer to this problem in the present section we explore more interesting configurations, including heterogeneities in the characteristic SW distance (Section 4.1) and in the initial shear stress (Section 4.2)

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Summary

Introduction

It is well known that numerical experiments represent, in addition to theory and to laboratory experiments, a suitable way to explore natural phenomena. One of the outcomes of realistic numerical experiments is that the direction of the fault slip (namely, the azimuth of the fault slip vector) can vary during the dynamic propagation of an earthquake rupture, even in homogeneous conditions. This phenomenon, named rake rotation, appears both in the time domain (in a given fault node the slip direction changes as long as the rupture dynamically propagates) and in the spatial domain (at a given time the slip direction is not the same over the slipping portions of the fault). Bizzarri and Cocco [2005] show that, even if the strength parameter S is the same (namely, if the ratio between the strength excess and the dynamic stress drop is kept constant), the rake rotation is smaller if the absolute values of the stress levels increase (see their Figure 13)

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