Dynamic faulting under rate-dependent friction

We discuss the effects of rate-dependent friction on the propagation of seismic rupture on active faults. Several physicists using Burridge and Knopoff's box and spring model of faulting have proposed that fault complexity may arise from the spontaneous development of a self-similar stress distribution on the fault plane. If this model proves to be correct, it has important consequences for the origin of the complexity of seismic sources. In order to test these ideas on a more realistic earthquake model, we developed a new boundary integral equation method for studying rupture propagation along an antiplane fault in the presence of nonlinear rate-dependent friction. We study rupture dynamics of models with single and twin asperities. In our models, asperities are places on the fault with a higher value of prestress. Othewise all fault parameters are homogeneous. We show that for models with such asperities, a slip velocity weakening friction leads to the propagation of supersonic healing phases and to the spontaneous arrest of fracture if the prestress outside the asperities is low enough. For models with asperities, we can also observe narrow slip velocity pulses, qualitatively similar to the so-called Heaton pulses observed in some earthquake accelerograms. We also observe a complex distribution of stress after the rupture that depends on details of the initial distribution of asperities and on the details of the friction law.

[1]  Keiiti Aki,et al.  Fault plane with barriers: A versatile earthquake model , 1977 .

[2]  D. P. Schwartz,et al.  Fault behavior and characteristic earthquakes: Examples from the Wasatch and San Andreas Fault Zones , 1984 .

[3]  S. K. Singh,et al.  The 1985 Central Chile Earthquake: A Repeat of Previous Great Earthquakes in the Region? , 1986, Science.

[4]  B. V. Kostrov,et al.  An investigation of the complexity of the earthquake source time function using dynamic faulting models , 1988 .

[5]  Shamita Das,et al.  A numerical method for determination of source time functions for general three‐dimensional rupture propagation , 1980 .

[6]  Keiiti Aki,et al.  Seismicity simulation with a rate- and state-dependent friction law , 1986 .

[7]  Marc Bonnet,et al.  Modelling of dynamical crack propagation using time-domain boundary integral equations , 1992 .

[8]  J. Dieterich Time‐dependent friction as a possible mechanism for aftershocks , 1972 .

[9]  B. V. Kostrov,et al.  Selfsimilar problems of propagation of shear cracks , 1964 .

[10]  T. Heaton Evidence for and implications of self-healing pulses of slip in earthquake rupture , 1990 .

[11]  A. Ruina,et al.  Slip motion and stability of a single degree of freedom elastic system with rate and state dependent friction , 1984 .

[12]  Raul Madariaga,et al.  On the relation between seismic moment and stress drop in the presence of stress and strength heterogeneity , 1979 .

[13]  J. Rice Spatio‐temporal complexity of slip on a fault , 1993 .

[14]  P. Okubo Dynamic rupture modeling with laboratory‐derived constitutive relations , 1989 .

[15]  W. Brace,et al.  Stick-Slip as a Mechanism for Earthquakes , 1966, Science.

[16]  J. Brune Tectonic stress and the spectra of seismic shear waves from earthquakes , 1970 .

[17]  Unsteady Propagation of Longitudinal Shear Cracks , 1970 .

[18]  The numerical solution of certain integral equations with non-integrable kernels arising in the theory of crack propagation and elastic wave diffraction , 1969, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[19]  A. Ruina,et al.  Stability of Steady Frictional Slipping , 1983 .

[20]  Carlson,et al.  Mechanical model of an earthquake fault. , 1989, Physical review. A, General physics.

[21]  L. Knopoff,et al.  Model and theoretical seismicity , 1967 .

[22]  Hiroo Kanamori,et al.  Seismological aspects of the Guatemala Earthquake of February 4, 1976 , 1978 .