Modeling of the Perfectly Matched Layer Absorbing Boundaries and Intrinsic Attenuation in Explicit Finite-Element Methods

We present an implementation of the perfectly matched layer (pml) absorbing boundary conditions and modeling of intrinsic attenuation ( Q ) in explicit finite-element simulations of wave propagation. The finite-element method uses one integration point and an hourglass control scheme, which leads to an easy extension of the velocity-stress implementation of pml to the finite-element method. Numerical examples using both regular and irregular elements in the pml region show excellent results: very few reflections are observed from the boundary for both body waves and surface waves—far superior to the classic first-order absorbing boundaries. The one-point integration also gives rise to an easy incorporation of the coarse-grain approach for modeling Q (Day, 1998). We implement the coarse-grain method in a structured finite-element mesh straightforwardly. We also apply the coarse-grain method to a widely used, slightly unstructured finite-element mesh, where unstructured finite elements are only used in the vertical velocity transition zones. A linear combination of eight relaxation mechanisms is used to simulate the target attenuation model over a wide frequency range. The relaxation time and weight of each relaxation mechanism are distributed in a spatially periodic manner to the center of each element. Stress relaxations caused by anelastic material response are calculated from elastic strains in the element and redistributed to the nodal forces of the element. Numerical simulation of anelastic wave propagation in a layered velocity structure with very small Q s using both the structured mesh and the unstructured mesh show excellent agreement with the analytical solutions when the viscoelastic modulus is calculated by a harmonic average over the coarse-grain unit. Our scheme greatly expands the use of pml and the coarse-grain method for modeling Q , so that these methods can be used in a versatile and efficient finite-element formulation.

[1]  D. Komatitsch,et al.  Spectral-element simulations of global seismic wave propagation—I. Validation , 2002 .

[2]  S. E. Zarantonello,et al.  Large scale calculations of 3D elastic wave propagation in a complex geology , 1992, Proceedings Supercomputing '92.

[3]  B. Engquist,et al.  Absorbing boundary conditions for acoustic and elastic wave equations , 1977, Bulletin of the Seismological Society of America.

[4]  K. Hudnut,et al.  Fault Interactions and Large Complex Earthquakes in the Los Angeles Area , 2003, Science.

[5]  Christopher R. Bradley,et al.  Memory-Efficient Simulation of Anelastic Wave Propagation , 2001 .

[6]  Jeroen Tromp,et al.  A perfectly matched layer absorbing boundary condition for the second-order seismic wave equation , 2003 .

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

[8]  R. Higdon Absorbing boundary conditions for elastic waves , 1991 .

[9]  A. Chopra,et al.  Perfectly matched layers for transient elastodynamics of unbounded domains , 2004 .

[10]  M. Korn,et al.  Incorporation of attenuation into time-domain computations of seismic wave fields , 1987 .

[11]  J. Gillis,et al.  Methods in Computational Physics , 1964 .

[12]  Don L. Anderson,et al.  Velocity dispersion due to anelasticity; implications for seismology and mantle composition , 1976 .

[13]  Edward L. Wilson,et al.  Incompatible Displacement Models , 1973 .

[14]  O. Ghattas,et al.  Simulations of Long-Period Ground Motions during the 1995 Hyogoken-Nanbu ( Kobe ) Earthquake using 3 D Finite Element Method , 1998 .

[15]  James F. Doyle,et al.  The Spectral Element Method , 2020, Wave Propagation in Structures.

[16]  Pengcheng Liu,et al.  Efficient Modeling of Q for 3D Numerical Simulation of Wave Propagation , 2006 .

[17]  D. Komatitsch,et al.  The Spectral-Element Method, Beowulf Computing, and Global Seismology , 2002, Science.

[18]  Steven M. Day,et al.  Efficient simulation of constant Q using coarse-grained memory variables , 1998, Bulletin of the Seismological Society of America.

[19]  John Lysmer,et al.  A Finite Element Method for Seismology , 1972 .

[20]  Gaetano Festa,et al.  PML Absorbing Boundaries , 2003 .

[21]  D. Komatitsch,et al.  Spectral-element simulations of global seismic wave propagation: II. Three-dimensional models, oceans, rotation and self-gravitation , 2002 .

[22]  L. John,et al.  Finite dynamic model for infinite media , 1969 .

[23]  Ralph J. Archuleta,et al.  Three-dimensional numerical simulations of dynamic faulting in a half-space , 1978, Bulletin of the Seismological Society of America.

[24]  T. Belytschko,et al.  A uniform strain hexahedron and quadrilateral with orthogonal hourglass control , 1981 .

[25]  Hiroyuki Fujiwara,et al.  Finite-element Simulation of Seismic Ground Motion with a Voxel Mesh , 2004 .

[26]  C. Tsogka,et al.  Application of the perfectly matched absorbing layer model to the linear elastodynamic problem in anisotropic heterogeneous media , 2001 .

[27]  Efficient 3-D viscoelastic modeling with application to near‐surface land seismic data , 1998 .

[28]  J. Bérenger Three-Dimensional Perfectly Matched Layer for the Absorption of Electromagnetic Waves , 1996 .

[29]  Robert W. Graves,et al.  Stability and Accuracy Analysis of Coarse-Grain Viscoelastic Simulations , 2003 .

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

[31]  Kim B. Olsen,et al.  On the implementation of perfectly matched layers in a three‐dimensional fourth‐order velocity‐stress finite difference scheme , 2003 .

[32]  G. A. Frazier,et al.  Treatment of hourglass patterns in low order finite element codes , 1978 .

[33]  Warwick D. Smith The Application of Finite Element Analysis to Body Wave Propagation Problems , 2007 .

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

[35]  John B. Schneider,et al.  Application of the perfectly matched layer (PML) absorbing boundary condition to elastic wave propagation , 1996 .

[36]  D. Komatitsch,et al.  Simulations of Ground Motion in the Los Angeles Basin Based upon the Spectral-Element Method , 2004 .

[37]  Chrysoula Tsogka,et al.  Application of the PML absorbing layer model to the linear elastodynamic problem in anisotropic hete , 1998 .

[38]  J. Sochacki Absorbing boundary conditions for the elastic wave equations , 1988 .

[39]  Ronnie Kosloff,et al.  Wave propagation simulation in a linear viscoacoustic medium , 1988 .

[40]  Pengcheng Liu,et al.  Non-linear multiparameter inversion using a hybrid global search algorithm: applications in reflection seismology , 1995 .

[41]  Jean-Pierre Berenger,et al.  A perfectly matched layer for the absorption of electromagnetic waves , 1994 .

[42]  J. M. Kennedy,et al.  Hourglass control in linear and nonlinear problems , 1983 .

[43]  J. O. Hallquist,et al.  Recent developments in large-scale finite-element Lagrangian hydrocode technology. [Dyna 20/dyna 30 computer code] , 1981 .

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

[45]  M. Carcione,et al.  Wave propagation simulation in a linear viscoacoustic medium , 1997 .

[46]  O. Ghattas,et al.  LARGE-SCALE NORTHRIDGE EARTHQUAKE SIMULATION USING OCTREE-BASED MULTIRESOLUTION MESH METHOD , 2003 .

[47]  S. Day Three-dimensional simulation of spontaneous rupture: The effect of nonuniform prestress , 1982 .

[48]  Joakim O. Blanch,et al.  Viscoelastic finite-difference modeling , 1994 .

[49]  J. Bernard Minster,et al.  Numerical simulation of attenuated wavefields using a Padé approximant method , 1984 .

[50]  D. Komatitsch,et al.  Introduction to the spectral element method for three-dimensional seismic wave propagation , 1999 .

[51]  David R. O'Hallaron,et al.  Large-scale simulation of elastic wave propagation in heterogeneous media on parallel computers , 1998 .