2020
DOI: 10.1016/j.cma.2020.113352
|View full text |Cite
|
Sign up to set email alerts
|

Systematic development of upwind numerical fluxes for the space discontinuous Galerkin method applied to elastic wave propagation in anisotropic and heterogeneous media with physical interfaces

Abstract: This research work presents, within a unified and wave oriented variational framework, systematic development of upwind numerical fluxes for the space discontinuous Galerkin methods to model elastic wave propagation in multidimensional anisotropic media with discontinuous material properties. Both first-order velocity-stress and velocity-strain wave formulations are considered. The proposed approach allows the derivation of upwind numerical fluxes in a well structured and hierarchical way according to the degr… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
2
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
4
1
1

Relationship

0
6

Authors

Journals

citations
Cited by 8 publications
(2 citation statements)
references
References 26 publications
0
2
0
Order By: Relevance
“…The numerical model is based on the following system of conservation laws, composed of the balance equation of linear momentum with no source term and geometrical conservation laws: In system (32), the unknowns are respectively σ and v, the Cauchy stress tensor and the velocity vector. The solid domain presented in figure 9 is then discretized as a Cartesian grid of space step ∆x = 12.0µm, in such a way that the semi-discrete form of the above governing equations can be written by means of the discontinuous Galerkin (DG) first-order approximation [29,30,40]. Note that such a finite element size leads to good convergence properties for continuous Galerkin finite element schemes [41,42], which have the same (second-order) accuracy as the considered DG approach.…”
Section: Discretizationmentioning
confidence: 99%
See 1 more Smart Citation
“…The numerical model is based on the following system of conservation laws, composed of the balance equation of linear momentum with no source term and geometrical conservation laws: In system (32), the unknowns are respectively σ and v, the Cauchy stress tensor and the velocity vector. The solid domain presented in figure 9 is then discretized as a Cartesian grid of space step ∆x = 12.0µm, in such a way that the semi-discrete form of the above governing equations can be written by means of the discontinuous Galerkin (DG) first-order approximation [29,30,40]. Note that such a finite element size leads to good convergence properties for continuous Galerkin finite element schemes [41,42], which have the same (second-order) accuracy as the considered DG approach.…”
Section: Discretizationmentioning
confidence: 99%
“…At last, an explicit two-step second-order Runge-Kutta time-discretization is used to derive the discrete system. The reader interested in more details about formulation, implementation and stability of DG methods for anisotropic and piecewise homogeneous media should refer to references [30,40,43].…”
Section: Discretizationmentioning
confidence: 99%