Static and dynamic fracture analysis of 3D cracked orthotropic shells using XFEM method
Introduction
Various methods have been used to analyze cracked composite structures. Among the performed studies in this field, closed-form solutions to the fracture mechanics behaviour of such materials could be addressed [1], [2]. Some of these studies focused on stress and displacement fields around a linear crack on an inhomogeneous medium [3], [4], [5], [6].
Since most analytical solutions are applicable to limited geometries and boundary conditions, numerical techniques such as boundary element method [7], [8], and finite element method [9], [10], [11] have been proposed for fracture analysis of composites with complex geometries.
The extended finite element method is a powerful numerical method capable of solving cracked fields without the need for matching crack boundaries with edge elements or any change in the generated meshes. In this method, Heaviside enrichment functions are utilized to consider crack-tip discontinuity enrichment functions that evaluate the singular field around the crack tip. The XFEM was originally proposed by Belytschko and Black [12]. It was further developed by Daux et al. [13], Belytschko et al. [14], Sukumar et al. [15] and other researchers [16], [17], [18], [19], [20] for plate problems. It was then extended to shell-type structures by Areias and Belytschko [21], Wyart et al. [22] and Bayesteh and Mohammadi [23] for isotropic materials. This method was originally used for homogenous materials while it is further extended to orthotropic media. The method necessitates different crack tip enrichment functions derived based on analytical solutions derived for near crack tip displacement fields. Different analytical solutions have been proposed to be applied for the specific classes of orthotropic materials [24], [25], through the use of analytical displacement fields [26], [27], [28], [29], [30]. Asadpoure and Mohammadi [31] proposed a set of crack-tip enrichment functions for composite materials using a unified analytical formulation [2]. The XFEM adopted with the layer-wise method is studied and developed by Li et al. [32], [33], [34], [35], [36], [37].
Analytical solutions of the dynamic analysis of cracked anisotropic media has been developed by Viola et al. [26], Broberg [38], Lim et al. [1] and Nobile and Carloni [29]. As well, others utilized numerical methods such as boundary element solutions [7], [8] or finite element method [39] for analysis of cracked anisotropic media. Belytschko et al. [40] and Grégoire et al. [41] modelled dynamic crack propagation through the XFEM framework for isotropic materials. Motamedi and Mohammadi [42], [43], [44] adopted the XFEM method for dynamic analysis of cracked orthotropic plates.
This study investigates 3D analysis of cracked orthotropic shell structures under static and dynamic loading. For this purpose, a MATLAB stand-alone code is developed to solve and post-process the results of stress intensity factors for cracked orthotropic elements through XFEM method.
Section snippets
Shell element formulation
If a solid element used to model a shell structure, errors could occur in computing stiffness of element due to the large number of integration points selected from a small thickness compared to other dimensions of the element [45]. To maintain the simplicity of modelling structures with 3D geometries, the so-called degenerated shell element is used, and the finite element computations are mainly performed in the 2D plane of the element. However, the 3D properties are still considered for the
XFEM software
Authors have developed a MATLAB stand-alone programming package due to the limitations of the available commercial FEM packages like ABAQUS. The main limitations of available commercial software to model the structures in XFEM method are:
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Orthotropic cracked materials could not be solved with the XFEM method. Neither orthotropic shell nor solid elements are supported by commercial software.
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The accessible shell elements are failed to be considered by the XFEM method. Neither isotropic materials
Numerical examples
To verify the accuracy of the present results, different examples of 2D and 3D domains are considered. First, an orthotropic plate with a crack parallel to material axis of orthotropic, and another plate with a central inclined crack having different angles with respect to the material axis are studied. As well, a cylindrical orthotropic pipe containing a crack with different orientations is considered. The effect of fibre direction on the strength of the structure is also studied to enrich the
Conclusions
To study fracture behaviour of orthotropic materials, the analytical solutions proposed by researchers are limited to specific types of structures with special loading and boundary conditions. Although the solutions, which are based on the finite element method could overcome these deficiencies, for problems that consider the crack growth during loading procedure, the method is not robust because it is needed for the crack body to match the elements within each step. Also, the same issue exists
Declaration of Competing Interest
None.
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