2015
DOI: 10.1016/j.compstruct.2015.01.053
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An XFEM/CZM implementation for massively parallel simulations of composites fracture

Abstract: Because of their widely spread use in many industries, composites are the subject of many research campaigns. More particularly, the development of both accurate and flexible numerical models able to capture their intrinsically multiscale modes of failure is still a challenge. The standard finite element method typically requires intensive remeshing to adequately capture the geometry of the cracks and high accuracy is thus often sacrificed in favor of scalability, and vice versa. In an effort to preserve both … Show more

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Cited by 39 publications
(21 citation statements)
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“…This also holds for the thickness normal stress and the shear stress. It is important to note that stress r is only obtained with the curvature termw in Equation (27). Asw is taken from the last load increment, the computation must be done in two steps.…”
Section: Clamped Circular Shellmentioning
confidence: 99%
See 2 more Smart Citations
“…This also holds for the thickness normal stress and the shear stress. It is important to note that stress r is only obtained with the curvature termw in Equation (27). Asw is taken from the last load increment, the computation must be done in two steps.…”
Section: Clamped Circular Shellmentioning
confidence: 99%
“…Due to the plane strain boundary conditions, the stresses are independent of y. Without the curvature term w in (27), one obtains the linear solution for z . The deformed configuration for load factor = 5 is plotted in Figure 12.…”
Section: Inelastic Analysis Of a Sandwich Plate Stripmentioning
confidence: 99%
See 1 more Smart Citation
“…This is achieved by multiplying the bulk strong form (6)(7)(8) by the trial functions (wū, wp) ∈ C 0 (Ω i ), and by integrating by parts on each ply Ω i instead of performing this integration on the whole domain Ω as it is usually performed. Using the boundary conditions (8-10, 13 and 17) and definitions (11) of the jump and average operators across the interface Γ L i+1 i between the surfaces Γ Li and Γ Li+1 , see …”
Section: Weak Formulation Of the Problemmentioning
confidence: 99%
“…The use of cohesive zones within the plies using the extended finite element method, see e.g. [8], or the phantom node method [9] does not suffer from the loss of solution uniqueness.…”
Section: Introductionmentioning
confidence: 99%