Spectral-element method with an optimal mass matrix for seismic wave modelling

被引:2
作者
Liu, Shaolin [1 ,2 ]
Yang, Dinghui [3 ]
Xu, Xiwei [1 ]
Wang, Wenshuai [4 ]
Li, Xiaofan [5 ]
Meng, Xueli [1 ,4 ]
机构
[1] Natl Inst Nat Hazards, Minist Emergency Management China, Beijing, Peoples R China
[2] Chinese Acad Sci, Inst Geol & Geophys, State Key Lab Lithospher Evolut, Beijing, Peoples R China
[3] Tsinghua Univ, Dept Math Sci, Beijing 100084, Peoples R China
[4] Ningxia Univ, Sch Math & Stat, Yinchuan, Ningxia, Peoples R China
[5] China Univ Geosci, Inst Geophys & Geomat, Wuhan, Peoples R China
基金
中国国家自然科学基金;
关键词
Spectral-element method; numerical integration; seismic wave modelling; forward modelling; DISCONTINUOUS GALERKIN METHOD; FINITE-DIFFERENCE; PROPAGATION; SCHEME; DISPERSION; EQUATION; STABILITY; OPERATORS; DYNAMICS;
D O I
10.1080/08123985.2022.2043126
中图分类号
P3 [地球物理学]; P59 [地球化学];
学科分类号
0708 ; 070902 ;
摘要
The spectral-element method (SEM), which combines the flexibility of the finite element method (FEM) with the accuracy of spectral method, has been successfully applied to simulate seismic wavefields in geological models on different scales. One kind of SEMs that adopts orthogonal Legendre polynomials is widely used in seismology community. In the SEM with orthogonal Legendre polynomials, the Gauss-Lobatto-Legendre (GLL) quadrature rule is employed to calculate the integrals involved in the SEM leading to a diagonal mass matrix. However, the GLL quadrature rule can exactly approximate only integrals with a polynomial degree below 2N-1 (N is the interpolation order in space) and cannot exactly calculate those of polynomials with degree 2N involved in the mass matrix. Therefore, the error of the mass matrix originating from inexact numerical integration may reduce the accuracy of the SEM. To improve the SEM accuracy, we construct a least-squares objective function in terms of numerical and exact integrals to increase the accuracy of the GLL quadrature rule. Then, we utilise the conjugate gradient method to solve the objective function and obtain a set of optimal quadrature weights. The optimal mass matrix can be obtained simultaneously by utilising the GLL quadrature rule with optimal integration weights. The improvement in the numerical accuracy of the SEM with an optimal mass matrix (OSEM) is demonstrated by theoretical analysis and numerical examples.
引用
收藏
页码:683 / 693
页数:11
相关论文
共 50 条
[1]  
Aarts EHL, 1987, SIMULATED ANNEALING, P7, DOI DOI 10.1007/978-94-015-7744-1_2
[2]   An average-derivative optimal scheme for modeling of the frequency-domain 3D elastic wave equation [J].
Chen, Jing-Bo ;
Cao, Jian .
GEOPHYSICS, 2018, 83 (04) :T209-T234
[3]  
Cohen G., 2006, SOC IND APPL MATH, V38, P78
[4]  
De Basabe JD, 2007, GEOPHYSICS, V72, pT81, DOI 10.1190/1.2785O46
[5]   Stability of the high-order finite elements for acoustic or elastic wave propagation with high-order time stepping [J].
De Basabe, Jonas D. ;
Sen, Mrinal K. .
GEOPHYSICAL JOURNAL INTERNATIONAL, 2010, 181 (01) :577-590
[6]   The interior penalty discontinuous Galerkin method for elastic wave propagation: grid dispersion [J].
De Basabe, Jonas D. ;
Sen, Mrinal K. ;
Wheeler, Mary F. .
GEOPHYSICAL JOURNAL INTERNATIONAL, 2008, 175 (01) :83-93
[7]   An arbitrary high-order Discontinuous Galerkin method for elastic waves on unstructured meshes -: II.: The three-dimensional isotropic case [J].
Dumbser, Michael ;
Kaeser, Martin .
GEOPHYSICAL JOURNAL INTERNATIONAL, 2006, 167 (01) :319-336
[8]  
Fichtner A, 2011, ADV GEOPHYS ENV MECH, P1, DOI 10.1007/978-3-642-15807-0_1
[9]   THE PSEUDOSPECTRAL METHOD - ACCURATE REPRESENTATION OF INTERFACES IN ELASTIC WAVE CALCULATIONS [J].
FORNBERG, B .
GEOPHYSICS, 1988, 53 (05) :625-637
[10]   MODELING OF THE ACOUSTIC-WAVE EQUATION WITH TRANSFORM METHODS [J].
GAZDAG, J .
GEOPHYSICS, 1981, 46 (06) :854-859