Abstract

The extended Finite Element Method (XFEM) is derived from the traditional finite element method for discontinuous problems. It can simulate the behavior of cracks, which significantly improves the ability of finite element methods to simulate geotechnical and geological disaster problems. The integration of discontinuous enrichment functions in weak form and the ill-conditioning of the system equations are two major challenges in employing the XFEM in engineering applications. A mixed integration scheme is proposed in this paper to solve these problems. This integration scheme has a simple form and exhibits both the accuracy of the subcell integration method and the well-conditioning of a smeared integration method. The correctness and effectiveness of the proposed scheme were verified through a series of element analyses and two typical examples. For XFEM numerical simulations with unstructured meshes and arbitrary cracks/interfaces, this method guarantees the convergence of nonlinear iterations and yields correct results.

Highlights

  • The extended Finite Element Method (XFEM) is an excellent numerical method that can visually simulate discontinuous cracks/interfaces and their evolution without mesh regeneration

  • The mixed scheme converged to the given minimum error limit after 69 iterations, as shown in Figure 19; the subcell scheme did not converge within the Newton iterations due to the illconditioning. These results prove that the mixed integration scheme exhibits good convergence stability for strongly nonlinear problems with unstructured meshes

  • This study introduced a smeared integration method that can integrate the weak form of elements with discontinuous enrichment without element splitting

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Summary

INTRODUCTION

The extended Finite Element Method (XFEM) is an excellent numerical method that can visually simulate discontinuous cracks/interfaces and their evolution without mesh regeneration. Table 2; Figure 7 present comparisons of the stiffness matrix condition numbers obtained using smeared and subcell integration with different penalty coefficients and partition ratios. The mixed scheme converged to the given minimum error limit after 69 iterations, as shown in Figure 19; the subcell scheme did not converge within the Newton iterations due to the illconditioning These results prove that the mixed integration scheme exhibits good convergence stability for strongly nonlinear problems with unstructured meshes

CONCLUSION
Findings
DATA AVAILABILITY STATEMENT
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