Statistical physics model for the spatiotemporal evolution of faults

A statistical physics model is used to simulate antiplane shear deformation and rupture of a tectonic plate with heterogeneous material properties. Rupture occurs when the chosen state variable reaches a threshold value. After rupture, broken elements are instantaneously healed and retain the original material properties. We document the spatiotemporal evolution of the rupture pattern in response to a constant velocity boundary condition. A fundamental feature of this model is that ruptures become strongly correlated in space and time, leading to the development of complex fractal structures. These structures, or “faults,” are simply defined by the loci where deformation accumulates. Repeated rupture of a fault occurs in events (“earthquakes”) which themselves exhibit both spatial and temporal clustering. Furthermore, we observe that a fault may be active for long periods of time until the locus of activity spontaneously switches to a different fault. The formation of the faults and the temporal variation of rupture activity is due to a complex interplay between the random small-scale structure, long-range elastic interactions, and the threshold nature of rupture physics. The characteristics of this scalar model suggest that spontaneous self-organization of active tectonics does not result solely from the tensorial nature of crustal deformation; that is, kinematic compatibility is not required for complex fault pattern formation. Furthermore, the localization of the deformation is a dynamical effect rather than a consequence of preexisting structure or preferential weakening of faults compared to the surrounding medium. We present an analysis of scaling relationships exhibited by the fault pattern and the earthquakes in this model.

[1]  J. Walsh,et al.  Analysis of the relationship between displacements and dimensions of faults , 1988 .

[2]  Javier F. Pacheco,et al.  Changes in frequency–size relationship from small to large earthquakes , 1992, Nature.

[3]  Patience A. Cowie,et al.  Physical explanation for the displacement-length relationship of faults using a post-yield fracture mechanics model , 1992 .

[4]  Christopher H. Scholz,et al.  Theory of time-dependent rupture in the Earth , 1981 .

[5]  Didier Sornette,et al.  Linking short-timescale deformation to long-timescale tectonics , 1992, Nature.

[6]  Geoffrey C. P. King,et al.  The accommodation of large strains in the upper lithosphere of the earth and other solids by self-similar fault systems: the geometrical origin of b-Value , 1983 .

[7]  Christensen,et al.  Self-organized criticality in a continuous, nonconservative cellular automaton modeling earthquakes. , 1992, Physical review letters.

[8]  Randall Marrett,et al.  Estimates of strain due to brittle faulting : sampling of fault populations , 1991 .

[9]  Didier Sornette,et al.  Fault growth in brittle‐ductile experiments and the mechanics of continental collisions , 1993 .

[10]  C. Scholz,et al.  Dilatancy in the fracture of crystalline rocks , 1966 .

[11]  P. Grassberger,et al.  Characterization of Strange Attractors , 1983 .

[12]  Sornette,et al.  Growth of fractal fault patterns. , 1990, Physical review letters.

[13]  C. Scholz,et al.  Fault growth and fault scaling laws: Preliminary results , 1993 .

[14]  P. Bak,et al.  Earthquakes as a self‐organized critical phenomenon , 1989 .

[15]  Patience A. Cowie,et al.  Displacement-length scaling relationship for faults: data synthesis and discussion , 1992 .

[16]  Noelle E. Odling,et al.  Network properties of a two-dimensional natural fracture pattern , 1992 .

[17]  Barbara Romanowicz,et al.  Strike‐slip earthquakes on quasi‐vertical transcurrent faults: Inferences for general scaling relations , 1992 .

[18]  Didier Sornette,et al.  The dynamical thermal fuse model , 1992 .

[19]  Christopher H. Scholz,et al.  Scaling laws for large earthquakes: Consequences for physical models , 1982 .

[20]  Self-organized ruptures in an elastic medium: a possible model for earthquakes , 1992 .

[21]  John B. Rundle,et al.  On scaling relations for large earthquakes , 1993, Bulletin of the Seismological Society of America.

[22]  Nakanishi Statistical properties of the cellular-automaton model for earthquakes. , 1991, Physical review. A, Atomic, molecular, and optical physics.

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

[24]  Distributed deformation and block rotation in three dimensions , 1991 .

[25]  Sornette,et al.  Dynamics and memory effects in rupture of thermal fuse networks. , 1992, Physical review letters.

[26]  A. Hansen,et al.  Introduction to Multifractality , 1990 .

[27]  Obukhov,et al.  Self-organized criticality in a crack-propagation model of earthquakes. , 1991, Physical review. A, Atomic, molecular, and optical physics.

[28]  L. Knopoff,et al.  Models of aftershock occurrence , 1987 .

[29]  J. Watterson Fault dimensions, displacements and growth , 1986 .

[30]  L. Sykes Aftershock zones of great earthquakes, seismicity gaps, and earthquake prediction for Alaska and the Aleutians , 1971 .

[31]  D. Sornette,et al.  Organization of Rupture , 1993 .

[32]  Takashi Nakata,et al.  Time‐predictable recurrence model for large earthquakes , 1980 .

[33]  S. Redner,et al.  A random fuse model for breaking processes , 1985 .

[34]  P. Gillespie,et al.  Limitations of dimension and displacement data from single faults and the consequences for data analysis and interpretation , 1992 .

[35]  Didier Sornette,et al.  Self-Organized Criticality and Earthquakes , 1989 .

[36]  Sornette,et al.  Statistical model of earthquake foreshocks. , 1992, Physical review. A, Atomic, molecular, and optical physics.

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

[38]  Patience A. Cowie,et al.  Determination of total strain from faulting using slip measurements , 1990, Nature.

[39]  D. Sornette,et al.  Structuration of the lithosphere in plate tectonics as a self‐organized critical phenomenon , 1990 .

[40]  Nakanishi Cellular-automaton model of earthquakes with deterministic dynamics. , 1990, Physical review. A, Atomic, molecular, and optical physics.