Off-fault plasticity in three-dimensional dynamic rupture simulations using a modal Discontinuous Galerkin method on unstructured meshes: implementation, verification and application

The dynamics and potential size of earthquakes depend crucially on rupture transfers between adjacent fault segments. To accurately describe earthquake source dynamics, numerical models can account for realistic fault geometries and rheologies such as nonlinear inelastic processes off the slip interface. We present implementation, verification and application of off-fault Drucker-Prager plasticity in the open source software SeisSol (www.seissol.org). SeisSol is based on an arbitrary high-order derivative modal Discontinuous Galerkin method using unstructured, tetrahedral meshes specifically suited for complex geometries. Two implementation approaches are detailed, modelling plastic failure either employing subelemental quadrature points or switching to nodal basis coefficients. At fine fault discretizations, the nodal basis approach is up to six times more efficient in terms of computational costs while yielding comparable accuracy. Both methods are verified in community benchmark problems and by 3-D numerical h-and p-refinement studies with heterogeneous initial stresses. We observe no spectral convergence for on-fault quantities with respect to a given reference solution, but rather discuss a limitation to low-order convergence for heterogeneous 3-D dynamic rupture problems. For simulations including plasticity, a high fault resolution may be less crucial than commonly assumed, due to the regularization of peak slip rate and an increase of the minimum cohesive zone width. In large-scale dynamic rupture simulations based on the 1992 Landers earthquake, we observe high rupture complexity including reverse slip, direct branching and dynamic triggering. The spatiotemporal distribution of rupture transfers are altered distinctively by plastic energy absorption, correlated with locations of geometrical fault complexity. Computational cost increases by 7 per cent when accounting for off-fault plasticity in the demonstrating application. Our results imply that the combination of fully 3-D dynamic modelling, complex fault geometries and off-fault plastic yielding is important to realistically capture dynamic rupture transfers in natural fault systems.

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

[2]  Michael Bader,et al.  Petascale Local Time Stepping for the ADER-DG Finite Element Method , 2016, 2016 IEEE International Parallel and Distributed Processing Symposium (IPDPS).

[3]  D. Andrews Rupture dynamics with energy loss outside the slip zone , 2003 .

[4]  Luis A. Dalguer,et al.  Asymmetric rupture of large aspect‐ratio faults at bimaterial interface in 3D , 2009 .

[5]  Steven G. Wesnousky,et al.  Seismological and structural evolution of strike-slip faults , 1988, Nature.

[6]  Leonhard Rannabauer,et al.  High-Order ADER-DG Minimizes Energy- and Time-to-Solution of SeisSol , 2015, ISC.

[7]  Michael Dumbser,et al.  Quadrature-free non-oscillatory finite volume schemes on unstructured meshes for nonlinear hyperbolic systems , 2007, J. Comput. Phys..

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

[9]  D. Sandwell,et al.  Three-dimensional deformation caused by the Bam, Iran, earthquake and the origin of shallow slip deficit , 2005, Nature.

[10]  Andrea Bizzarri,et al.  How to Promote Earthquake Ruptures: Different Nucleation Strategies in a Dynamic Model with Slip-Weakening Friction , 2010 .

[11]  Martin Käser,et al.  Quantitative accuracy analysis of the discontinuous Galerkin method for seismic wave propagation , 2008 .

[12]  Arash Khosravifar,et al.  A finite difference method for off-fault plasticity throughout the earthquake cycle , 2017 .

[13]  Shuo Ma,et al.  Distinct asymmetry in rupture‐induced inelastic strain across dipping faults: An off‐fault yielding model , 2009 .

[14]  Edward J. Hyer,et al.  Late summer changes in burning conditions in the boreal regions and their implications for NOx and CO emissions from boreal fires , 2008 .

[15]  Michael Barall,et al.  Metrics for Comparing Dynamic Earthquake Rupture Simulations , 2015 .

[16]  Tomokazu Kobayashi,et al.  Dynamic rupture propagation on geometrically complex fault with along-strike variation of fault maturity: insights from the 2014 Northern Nagano earthquake , 2017, Earth, Planets and Space.

[17]  L. J. Sluys,et al.  Interaction between material length scale and imperfection size for localisation phenomena in viscoplastic media , 1996 .

[18]  Harsha S. Bhat,et al.  Effect of Brittle Off‐Fault Damage on Earthquake Rupture Dynamics , 2017 .

[19]  Michel Campillo,et al.  Contribution of radar interferometry to a two-step inversion of the kinematic process of the 1992 Landers earthquake , 1999 .

[20]  P. Mai,et al.  Source properties of dynamic rupture pulses with off‐fault plasticity , 2013 .

[21]  Xiaohua Xu,et al.  Refining the shallow slip deficit , 2016 .

[22]  M. Dumbser,et al.  An arbitrary high-order discontinuous Galerkin method for elastic waves on unstructured meshes - I. The two-dimensional isotropic case with external source terms , 2006 .

[23]  B. Duan,et al.  Heterogeneous fault stresses from previous earthquakes and the effect on dynamics of parallel strike‐slip faults , 2006 .

[24]  Raul Madariaga,et al.  On the Self-Healing Fracture Mode , 2003 .

[25]  Y. Fialko Probing the mechanical properties of seismically active crust with space geodesy: Study of the coseismic deformation due to the 1992 Mw7.3 Landers (southern California) earthquake , 2004 .

[26]  Kenneth Duru,et al.  Dynamic earthquake rupture simulations on nonplanar faults embedded in 3D geometrically complex, heterogeneous elastic solids , 2016, J. Comput. Phys..

[27]  Michel Campillo,et al.  Frequency domain inversion of strong motions: Application to the 1992 Landers earthquake , 1995 .

[28]  A. Stroud Approximate calculation of multiple integrals , 1973 .

[29]  Michael Dumbser,et al.  Arbitrary high order accurate space-time discontinuous Galerkin finite element schemes on staggered unstructured meshes for linear elasticity , 2018, J. Comput. Phys..

[30]  Luis A. Dalguer,et al.  Staggered-grid split-node method for spontaneous rupture simulation , 2007 .

[31]  B. Duan,et al.  Asymmetric off‐fault damage generated by bilateral ruptures along a bimaterial interface , 2008 .

[32]  A. Pitarka,et al.  The SCEC/USGS Dynamic Earthquake Rupture Code Verification Exercise , 2012 .

[33]  Yehuda Ben-Zion,et al.  Characterization of Fault Zones , 2003 .

[34]  Harold L. Atkins,et al.  QUADRATURE-FREE IMPLEMENTATION OF DISCONTINUOUS GALERKIN METHOD FOR HYPERBOLIC EQUATIONS , 1996 .

[35]  Michael Barall,et al.  A grid‐doubling finite‐element technique for calculating dynamic three‐dimensional spontaneous rupture on an earthquake fault , 2009 .

[36]  Steven G. Wesnousky,et al.  Predicting the endpoints of earthquake ruptures , 2006, Nature.

[37]  E. Toro Riemann Solvers and Numerical Methods for Fluid Dynamics , 1997 .

[38]  J. C. Simo,et al.  Non‐smooth multisurface plasticity and viscoplasticity. Loading/unloading conditions and numerical algorithms , 1988 .

[39]  J. Rice,et al.  Off-fault plasticity and earthquake rupture dynamics: 1. Dry materials or neglect of fluid pressure changes , 2008 .

[40]  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 .

[41]  V. Dias da Silva,et al.  A simple model for viscous regularization of elasto‐plastic constitutive laws with softening , 2004 .

[42]  Christian Pelties,et al.  On the initiation of sustained slip-weakening ruptures by localized stresses , 2015 .

[43]  R. Borst,et al.  Non-Associated Plasticity for Soils, Concrete and Rock , 1984 .

[44]  Sebastien Leprince,et al.  Quantifying near‐field and off‐fault deformation patterns of the 1992 Mw 7.3 Landers earthquake , 2015 .

[45]  David D. Pollard,et al.  Impacts of off‐fault plasticity on fault slip and interaction at the base of the seismogenic zone , 2017 .

[46]  Suzanne M. Carbotte,et al.  Magmatic subsidence of the East Pacific Rise (EPR) at 18°14′S revealed through fault restoration of ridge crest bathymetry , 2003 .

[47]  Wei Zhang,et al.  Three-dimensional curved grid finite-difference modelling for non-planar rupture dynamics , 2014 .

[48]  Luis A. Dalguer,et al.  Dynamic earthquake rupture modelled with an unstructured 3-D spectral element method applied to the 2011 M9 Tohoku earthquake , 2014 .

[49]  Alice-Agnes Gabriel,et al.  Sustained Petascale Performance of Seismic Simulations with SeisSol on SuperMUC , 2014, ISC.

[50]  David D. Pollard,et al.  Mechanics of nonplanar faults at extensional steps with application to the 1992 M 7.3 Landers, California, earthquake , 2013 .

[51]  Andrea Bizzarri,et al.  Mechanics of 3-D shear cracks between Rayleigh and shear wave rupture speeds , 2012 .

[52]  Ralph J. Archuleta,et al.  The Three-Dimensional Dynamics of Dipping Faults , 2000 .

[53]  Yoshiaki Ida,et al.  The maximum acceleration of seismic ground motion , 1973 .

[54]  Luis A. Dalguer,et al.  Rupture Reactivation during the 2011 Mw 9.0 Tohoku Earthquake: Dynamic Rupture and Ground‐Motion Simulations , 2016 .

[55]  Yehuda Ben-Zion,et al.  Properties of inelastic yielding zones generated by in-plane dynamic ruptures—I. Model description and basic results , 2011 .

[56]  D. Pollard,et al.  Integration of Surface Slip and Aftershocks to Constrain the 3D Structure of Faults Involved in the M 7.3 Landers Earthquake, Southern California , 2012 .

[57]  Jean-Paul Ampuero,et al.  Pulse-like ruptures induced by low-velocity fault zones , 2011 .

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

[59]  John R. Rice,et al.  Finite Element Modeling of Branched Ruptures Including Off‐Fault Plasticity , 2012 .

[60]  Jens Oeser Entwicklung integrierter IT-Infrastrukturen für die Simulation komplexer geophysikalischer Prozesse , 2009 .

[61]  Alice-Agnes Gabriel,et al.  ASAGI: A Parallel Server for Adaptive Geoinformation , 2016, EASC.

[62]  H. Aochi,et al.  Spontaneous Rupture Propagation on a Non-planar Fault in 3-D Elastic Medium , 2000 .

[63]  Pradeep Dubey,et al.  High Order Seismic Simulations on the Intel Xeon Phi Processor (Knights Landing) , 2016, ISC.

[64]  T. Hanks,et al.  Verifying a Computational Method for Predicting Extreme Ground Motion , 2011 .

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

[66]  Yuri Fialko,et al.  Shallow slip deficit due to large strike-slip earthquakes in dynamic rupture simulations with elasto-plastic off-fault response , 2011 .

[67]  Hideo Aochi,et al.  Three‐dimensional nonplanar simulation of the 1992 Landers earthquake , 2002 .

[68]  Francisco J. Sánchez-Sesma,et al.  A 3D hp‐adaptive discontinuous Galerkin method for modeling earthquake dynamics , 2012 .

[69]  Georg Stadler,et al.  A high-order discontinuous Galerkin method for wave propagation through coupled elastic-acoustic media , 2010, J. Comput. Phys..

[70]  Kim B. Olsen,et al.  Off‐fault deformations and shallow slip deficit from dynamic rupture simulations with fault zone plasticity , 2017 .

[71]  Chi-Wang Shu,et al.  Discontinuous Galerkin Methods: Theory, Computation and Applications , 2011 .

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

[73]  R. LeVeque Finite Volume Methods for Hyperbolic Problems: Characteristics and Riemann Problems for Linear Hyperbolic Equations , 2002 .

[74]  GEOFFREY KING,et al.  Role of Fault Bends in the Initiation and Termination of Earthquake Rupture , 1985, Science.

[75]  Eleuterio F. Toro,et al.  ADER: Arbitrary High Order Godunov Approach , 2002, J. Sci. Comput..

[76]  Emanuele Casarotti,et al.  Forward and adjoint simulations of seismic wave propagation on fully unstructured hexahedral meshes , 2011 .

[77]  Ares J. Rosakis,et al.  Finite element simulations of dynamic shear rupture experiments and dynamic path selection along kinked and branched faults , 2009 .

[78]  S. Day,et al.  Inelastic strain distribution and seismic radiation from rupture of a fault kink , 2008 .

[79]  Steven M. Day,et al.  Stochastic Fault Stress: Implications for Fault Dynamics and Ground Motion , 2002 .

[80]  D. Fäh,et al.  Expected seismic shaking in Los Angeles reduced by San Andreas fault zone plasticity , 2014 .

[81]  D. J. Andrews,et al.  Test of two methods for faulting in finite-difference calculations , 1999 .

[82]  S. Somala,et al.  A Suite of Exercises for Verifying Dynamic Earthquake Rupture Codes , 2018 .

[83]  Y. Ben‐Zion,et al.  Damage-breakage rheology model and solid-granular transition near brittle instability , 2014 .

[84]  Shuo Ma,et al.  Inelastic off-fault response and three-dimensional dynamics of earthquake rupture on a strike-slip fault , 2010 .

[85]  Tim Warburton,et al.  An explicit construction of interpolation nodes on the simplex , 2007 .

[86]  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..

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

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

[89]  D. Wald,et al.  Spatial and temporal distribution of slip for the 1992 Landers, California, earthquake , 1994, Bulletin of the Seismological Society of America.

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

[91]  Robyn Hannigan,et al.  Evolving east Asian river systems reconstructed by trace element and Pb and Nd isotope variations in modern and ancient Red River‐Song Hong sediments , 2008 .

[92]  Ryosuke Ando Fast Domain Partitioning Method for dynamic boundary integral equations applicable to non-planar faults dipping in 3-D elastic half-space , 2016 .

[93]  Jeremy E. Kozdon,et al.  Simulation of Earthquake Rupture Dynamics in Complex Geometries Using Coupled Finite Difference and Finite Volume Methods , 2015 .

[94]  Lilia Krivodonova,et al.  Limiters for high-order discontinuous Galerkin methods , 2007, J. Comput. Phys..

[95]  Jean-Paul Ampuero,et al.  Earthquake source characteristics from dynamic rupture with constrained stochastic fault stress , 2007 .

[96]  J. Hesthaven,et al.  Nodal Discontinuous Galerkin Methods: Algorithms, Analysis, and Applications , 2007 .

[97]  J. Lions,et al.  Inequalities in mechanics and physics , 1976 .

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

[99]  J. D. Platt,et al.  Steadily propagating slip pulses driven by thermal decomposition , 2015 .

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

[101]  Christophe Geuzaine,et al.  Gmsh: A 3‐D finite element mesh generator with built‐in pre‐ and post‐processing facilities , 2009 .

[102]  Yehuda Ben-Zion,et al.  Dynamic rupture in a damage-breakage rheology model , 2016 .

[103]  Alice-Agnes Gabriel,et al.  Verification of an ADER-DG method for complex dynamic rupture problems , 2013 .

[104]  A. Pitarka,et al.  Broadband Ground-Motion Simulation Using a Hybrid Approach , 2010 .

[105]  Donald B. Campbell,et al.  Mercury's moment of inertia from spin and gravity data , 2012 .

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

[107]  Michael Ortiz,et al.  An analysis of a new class of integration algorithms for elastoplastic constitutive relations , 1986 .

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

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

[110]  James P. Evans,et al.  Internal structure and weakening mechanisms of the San Andreas Fault , 1993 .

[111]  Yoshiaki Ida,et al.  Cohesive force across the tip of a longitudinal‐shear crack and Griffith's specific surface energy , 1972 .

[112]  N. Takegawa,et al.  Rapid aerosol particle growth and increase of cloud condensation nucleus activity by secondary aerosol formation and condensation: A case study for regional air pollution in northeastern China , 2009 .

[113]  Kim B. Olsen,et al.  Quantification of Fault-Zone Plasticity Effects with Spontaneous Rupture Simulations , 2017, Pure and Applied Geophysics.

[114]  T. Mitchell,et al.  The nature and origin of off-fault damage surrounding strike-slip fault zones with a wide range of displacements: A field study from the Atacama fault system, northern Chile , 2009 .

[115]  Hideo Aochi,et al.  Constraint of fault parameters inferred from nonplanar fault modeling , 2003 .

[116]  M. Y. Hussaini,et al.  An Analysis of the Discontinuous Galerkin Method for Wave Propagation Problems , 1999 .

[117]  M. V. de Hoop,et al.  Imaging of structure at and near the core-mantle boundary using a generalized radon transform: 2. Statistical inference of singularities , 2007 .

[118]  Shuo Ma A physical model for widespread near‐surface and fault zone damage induced by earthquakes , 2008 .

[119]  Kenneth Duru,et al.  A new discontinuous Galerkin spectral element method for elastic waves with physically motivated numerical fluxes , 2018, 1802.06380.

[120]  P. Roache Code Verification by the Method of Manufactured Solutions , 2002 .

[121]  Sonia Fliss,et al.  Fault branching and rupture directivity , 2002 .

[122]  Luis A. Dalguer,et al.  Modelling of rupture propagation using high‐order mimetic finite differences , 2008 .

[123]  Yehuda Ben-Zion,et al.  Dynamic Ruptures on a Frictional Interface with Off-Fault Brittle Damage: Feedback Mechanisms and Effects on Slip and Near-Fault Motion , 2015, Pure and Applied Geophysics.

[124]  Kojiro Irikura,et al.  Simulation of tensile crack generation by three-dimensional dynamic shear rupture propagation during an earthquake , 2003 .

[125]  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 .

[126]  E. Hauksson,et al.  The 1992 Landers Earthquake Sequence: Seismological observations , 1993 .

[127]  M. Dumbser,et al.  An arbitrary high-order discontinuous Galerkin method for elastic waves on unstructured meshes — II. The three-dimensional isotropic case , 2006 .

[128]  R. Madariaga,et al.  Dynamic modeling of the 1992 Landers earthquake , 2001 .