Simulation of Dynamic Earthquake Ruptures in Complex Geometries Using High-Order Finite Difference Methods

We develop a stable and high-order accurate finite difference method for problems in earthquake rupture dynamics in complex geometries with multiple faults. The bulk material is an isotropic elastic solid cut by pre-existing fault interfaces that accommodate relative motion of the material on the two sides. The fields across the interfaces are related through friction laws which depend on the sliding velocity, tractions acting on the interface, and state variables which evolve according to ordinary differential equations involving local fields.The method is based on summation-by-parts finite difference operators with irregular geometries handled through coordinate transforms and multi-block meshes. Boundary conditions as well as block interface conditions (whether frictional or otherwise) are enforced weakly through the simultaneous approximation term method, resulting in a provably stable discretization.The theoretical accuracy and stability results are confirmed with the method of manufactured solutions. The practical benefits of the new methodology are illustrated in a simulation of a subduction zone megathrust earthquake, a challenging application problem involving complex free-surface topography, nonplanar faults, and varying material properties.

[1]  Jan Nordström,et al.  High-order finite difference methods, multidimensional linear problems, and curvilinear coordinates , 2001 .

[2]  C. Marone LABORATORY-DERIVED FRICTION LAWS AND THEIR APPLICATION TO SEISMIC FAULTING , 1998 .

[3]  Jan Nordström,et al.  Conservative Finite Difference Formulations, Variable Coefficients, Energy Estimates and Artificial Dissipation , 2006, J. Sci. Comput..

[4]  Eli Turkel,et al.  A fourth-order accurate finite-difference scheme for the computation of elastic waves , 1986 .

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

[6]  Takashi Miyatake,et al.  NUMERICAL SIMULATIONS OF EARTHQUAKE SOURCE PROCESS BY A THREE-DIMENSIONAL CRACK MODEL. , 1980 .

[7]  Magnus Svärd,et al.  On the order of accuracy for difference approximations of initial-boundary value problems , 2006, J. Comput. Phys..

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

[9]  S. Day,et al.  Comparison of finite difference and boundary integral solutions to three‐dimensional spontaneous rupture , 2005 .

[10]  Ken Mattsson,et al.  Summation by Parts Operators for Finite Difference Approximations of Second-Derivatives with Variable Coefficients , 2012, J. Sci. Comput..

[11]  Alfred Behle,et al.  Elastic wave propagation simulation in the presence of surface topography , 1992 .

[12]  Steven M. Day,et al.  Three-dimensional finite difference simulation of fault dynamics: Rectangular faults with fixed rupture velocity , 1982 .

[13]  Stefan Nilsson,et al.  Stable Difference Approximations for the Elastic Wave Equation in Second Order Formulation , 2007, SIAM J. Numer. Anal..

[14]  E. Dunham,et al.  Earthquake Ruptures with Strongly Rate-Weakening Friction and Off-Fault Plasticity, Part 1: Planar Faults , 2011 .

[15]  D. Gottlieb,et al.  Time-stable boundary conditions for finite-difference schemes solving hyperbolic systems: methodology and application to high-order compact schemes , 1994 .

[16]  D. J. Andrews,et al.  Rupture propagation with finite stress in antiplane strain , 1976 .

[17]  Martin Käser,et al.  Dynamic rupture modeling on unstructured meshes using a discontinuous Galerkin method , 2009 .

[18]  M. Carpenter,et al.  Fourth-order 2N-storage Runge-Kutta schemes , 1994 .

[19]  Narumi Takahashi,et al.  Structural characteristics off Miyagi forearc region, the Japan Trench seismogenic zone, deduced from a wide-angle reflection and refraction study , 2005 .

[20]  Timothy G. Trucano,et al.  Verification and validation. , 2005 .

[21]  H. Kreiss Initial boundary value problems for hyperbolic systems , 1970 .

[22]  J. Rice,et al.  Elastodynamic analysis for slow tectonic loading with spontaneous rupture episodes on faults with rate‐ and state‐dependent friction , 2000 .

[23]  S. Das Numerical method for determination of source time functions for general three dimensional rupture propagation : Geophys J R Astr Soc, V62, N3, Sept 1980, P591–604 , 1981 .

[24]  Jeremy E. Kozdon,et al.  Interaction of Waves with Frictional Interfaces Using Summation-by-Parts Difference Operators: Weak Enforcement of Nonlinear Boundary Conditions , 2012, J. Sci. Comput..

[25]  Sarah E. Minson,et al.  The 2011 Magnitude 9.0 Tohoku-Oki Earthquake: Mosaicking the Megathrust from Seconds to Centuries , 2011, Science.

[26]  Luis A. Dalguer,et al.  Finite difference modelling of rupture propagation with strong velocity-weakening friction , 2009 .

[27]  Gutuan Zheng,et al.  Self-healing slip pulse on a frictional surface , 1995 .

[28]  Hideo Aochi,et al.  Selectivity of spontaneous rupture propagation on a branched fault , 2000 .

[29]  Olsson,et al.  SUMMATION BY PARTS, PROJECTIONS, AND STABILITY. I , 2010 .

[30]  D. J. Andrews,et al.  Bulletin of the Seismological Society of America , 1985 .

[31]  H. Kreiss,et al.  Finite Element and Finite Difference Methods for Hyperbolic Partial Differential Equations , 1974 .

[32]  Xiaofei Chen,et al.  Dynamic rupture process of the 1999 Chi-Chi, Taiwan, earthquake , 2009 .

[33]  R. Madariaga,et al.  Modeling Dynamic Rupture in a 3 D Earthquake Fault Model by , 1998 .

[34]  J. Vilotte,et al.  The Newmark scheme as velocity–stress time-staggering: an efficient PML implementation for spectral element simulations of elastodynamics , 2005 .

[35]  P. Olsson Summation by parts, projections, and stability. II , 1995 .

[36]  Gunilla Kreiss,et al.  Perfectly Matched Layers for Hyperbolic Systems: General Formulation, Well-posedness, and Stability , 2006, SIAM J. Appl. Math..

[37]  Bengt Fornberg,et al.  The pseudospectral method; accurate representation of interfaces in elastic wave calculations , 1988 .

[38]  J. Rice,et al.  Rate and state dependent friction and the stability of sliding between elastically deformable solids , 2001 .

[39]  Narumi Takahashi,et al.  Seismic structure and seismogenesis off Sanriku region, northeastern Japan , 2004 .

[40]  J. Kristek,et al.  The finite-difference and finite-element modeling of seismic wave propagation and earthquake motion , 2007 .

[41]  Narumi Takahashi,et al.  Tectonic features of the Japan Trench convergent margin off Sanriku, northeastern Japan, revealed by multichannel seismic reflection data , 2000 .

[42]  R. Madariaga,et al.  Modeling dynamic rupture in a 3D earthquake fault model , 1998, Bulletin of the Seismological Society of America.

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

[44]  Nobuki Kame,et al.  Simulation of the spontaneous growth of a dynamic crack without constraints on the crack tip path , 1999 .

[45]  Thomas H. Heaton,et al.  Dynamic Earthquake Ruptures in the Presence of Lithostatic Normal Stresses: Implications for Friction Models and Heat Production , 2001 .

[46]  J. Rice,et al.  A spectral method for three-dimensional elastodynamic fracture problems , 1995 .

[47]  J. Rice,et al.  Constitutive relations for fault slip and earthquake instabilities , 1983 .

[48]  Dan Givoli,et al.  High-order local absorbing conditions for the wave equation: Extensions and improvements , 2008, J. Comput. Phys..

[49]  J. Dieterich Modeling of rock friction: 1. Experimental results and constitutive equations , 1979 .

[50]  Patrick J. Roache,et al.  Verification and Validation in Computational Science and Engineering , 1998 .

[51]  Shuo Ma,et al.  Modeling of the Perfectly Matched Layer Absorbing Boundaries and Intrinsic Attenuation in Explicit Finite-Element Methods , 2006 .

[52]  Jeremy E. Kozdon,et al.  Earthquake Ruptures with Strongly Rate-Weakening Friction and Off-Fault Plasticity : 2 . Nonplanar Faults , 2010 .

[53]  William S. Slaughter The Linearized Theory of Elasticity , 2001 .

[54]  Oglesby,et al.  Earthquakes on dipping faults: the effects of broken symmetry , 1998, Science.

[55]  H. Kreiss,et al.  Initial-Boundary Value Problems and the Navier-Stokes Equations , 2004 .

[56]  B. Gustafsson The convergence rate for difference approximations to mixed initial boundary value problems , 1975 .

[57]  Gustavo Ponce Initial-Boundary Value Problems and the Navier-Stokes Equations (Heinz-Otto Kreiss and Jens Lorenz) , 1990, SIAM Rev..

[58]  Jean-Paul Ampuero Étude physique et numérique de la nucléation des séismes , 2002 .

[59]  D. Gottlieb,et al.  A Stable and Conservative Interface Treatment of Arbitrary Spatial Accuracy , 1999 .

[60]  Akira Asada,et al.  Displacement Above the Hypocenter of the 2011 Tohoku-Oki Earthquake , 2011, Science.

[61]  Jeremy E. Kozdon,et al.  Earthquake Ruptures with Strongly Rate-Weakening Friction and Off-Fault Plasticity, Part 2: Nonplanar FaultsEarthquake Ruptures with Rate-Weakening Friction and Off-Fault Plasticity, Part 2: Nonplanar Faults , 2011 .

[62]  A. Ruina Slip instability and state variable friction laws , 1983 .

[63]  L. E. Malvern Introduction to the mechanics of a continuous medium , 1969 .

[64]  Jeremy E. Kozdon,et al.  Rupture to the Trench: Dynamic Rupture Simulations of the 11 March 2011 Tohoku Earthquake , 2013 .

[65]  John R. Rice,et al.  Aseismic slip transients emerge spontaneously in three-dimensional rate and state modeling of subduction earthquake sequences , 2005 .

[66]  H. Kreiss,et al.  Time-Dependent Problems and Difference Methods , 1996 .

[67]  D. Appelö,et al.  A stable finite difference method for the elastic wave equation on complex geometries with free surfaces , 2007 .

[68]  J. Rice,et al.  Earthquake ruptures with thermal weakening and the operation of major faults at low overall stress levels , 2009 .

[69]  J. Nordström,et al.  Summation by Parts Operators for Finite Difference Approximations of Second-Derivatives with Variable Coefficients , 2004, Journal of Scientific Computing.

[70]  J. E. Kozdon,et al.  Rupture to the Trench in Dynamic Models of the Tohoku-Oki Earthquake , 2011 .

[71]  J. Ampuero,et al.  Spectral element modeling of spontaneous earthquake rupture on rate and state faults: Effect of velocity‐strengthening friction at shallow depths , 2008 .

[72]  J. Ampuero,et al.  Three‐dimensional dynamic rupture simulation with a high‐order discontinuous Galerkin method on unstructured tetrahedral meshes , 2012 .

[73]  Jean Virieux,et al.  Dynamic rupture simulation of non-planar faults with a finite-difference approach , 2004 .

[74]  B. Strand Summation by parts for finite difference approximations for d/dx , 1994 .

[75]  Patrick M. Knupp,et al.  Fundamentals of Grid Generation , 2020 .