Abstract

This paper presents an efficient hybrid asynchronous three-dimensional (3D) perfectly matched layer (PML) for modeling unbounded domains. The proposed unsplit explicit or implicit 3D PML formulation is implemented in the framework of a heterogeneous asynchronous time integrator. It is fully versatile in terms of time integrators and time step sizes according to partitions while conserving classical finite element formulations in the elastic domain without complex-valued stretched coordinates. Examples of a semi-infinite bar, Lamb’s test, and a soil–structure interaction problem with PML-truncated semi-infinite heterogeneous media are investigated to illustrate the efficiency of the proposed PML in terms of accuracy and CPU time.

Highlights

  • One of the critical issues regarding the numerical simulation of wave propagation problems in unbounded domains using the finite element method is finding a suitable technique to simulate infinite media

  • The present paper presents an efficient hybrid asynchronous 3D perfectly matched layer (PML) for modeling unbounded domains through a standard displacement-based finite element method, which is well suitable for finite element implementation

  • A novel 3D PML, which is suitable for finite element implementation, has been proposed in this paper for transient elastodynamics

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Summary

Introduction

One of the critical issues regarding the numerical simulation of wave propagation problems in unbounded domains using the finite element method is finding a suitable technique to simulate infinite media. The proposed unsplit 3D explicit/implicit PML formulation is implemented in the framework of a heterogeneous asynchronous time integrator (HATI) [22, 23], which employs the dual approach with Lagrange multipliers for subdomain coupling. This enables the PML to be treated independently using an explicit or implicit scheme with large time steps while conserving classical finite element formulations in the elastic domain to optimize computational efficiency. Various examples, including a 3D semi-infinite bar, Lamb’s test, and soil–structure interaction (SSI) with different soil layers, are investigated to illustrate the efficiency of the HATI formulation in terms of accuracy and CPU time

Design of a perfectly matched layer
Wave propagation from elastic medium to PML medium
Three-dimensional PML
Strong form of the three-dimensional PML
Weak form of the three-dimensional PML
Finite element discretization
Weak form for subdomain coupling
Multi-time-step implicit PML
Multi-time-step explicit PML
Interface problem
Numerical test of a semi-infinite 3D elastic bar
Findings
Conclusion
Full Text
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