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Civil-Comp Proceedings
ISSN 1759-3433 CCP: 83
PROCEEDINGS OF THE EIGHTH INTERNATIONAL CONFERENCE ON COMPUTATIONAL STRUCTURES TECHNOLOGY Edited by: B.H.V. Topping, G. Montero and R. Montenegro
Paper 266
Metis Element Model for Interlaminar Stresses in Composite Laminates N.T. Duong1 and H. Nguyen Dang2
1Welding and Metals' Technology Department, Hanoi University of Technology, Vietnam
N.T. Duong, H. Nguyen Dang, "Metis Element Model for Interlaminar Stresses in Composite Laminates", in B.H.V. Topping, G. Montero, R. Montenegro, (Editors), "Proceedings of the Eighth International Conference on Computational Structures Technology", Civil-Comp Press, Stirlingshire, UK, Paper 266, 2006. doi:10.4203/ccp.83.266
Keywords: metis element, interlaminar stresses, composite laminate, free edge.
Summary
The "metis" finite element method was developed by Nguyen Dang [1]. It is a
special class of hybrid finite element. The unisolvent condition of the external
displacement field permits the transformation of the integral of contour into an integral of
volume. This is a special class of the classic hybrid model. The present paper deals
with the use the "metis" displacement method to calculate the interlaminar stresses
in composite laminate structures. The results for the symmetric composite laminates
under a uniform axial strain are presented and compared to many other studies to
demonstrate the accuracy and efficiency of the present method.
Consider a composite material structure subjected to a constant axial extension. Several attempts have been made to obtain accurate stress distributions in this structure: finite element method, hybrid stress finite element, pure equilibrium, complex series expansion in conjunction with boundary collocation or singular hybrid finite element. This paper develops the metis displacement finite element method to solve this problem. Based on Lekhnitskii's elasticity theory [2], the formulae of generalized plane strain state for composite laminate structure are established. The problem in three dimensions is reduced to a problem in two and a half dimensions: The geometry is a two dimensional domain and the displacement and stress fields are in three dimensions. Then, we use the metis finite element method to establish the variational formulation for free edge problem of composite laminate. After that, the discretized formulation for metis displacement finite element is presented. In the metis element method, the Lagranges multiplier field, which is interpreted physically as the displacement field is prolonged to the interior of each element in a continuous manner (unisolvent principle). This principle permits the transformation of a contour integral into a volume integral or into a surface integral. In the application part of the paper, a composite laminate combined from four symmetrical layers of a high-modulus graphite-epoxy system is considered. The axial strain is assumed to be uniform. As a result of geometric symmetry, only a quarter of the cross sectional area is considered. The triangular element in second degree and a mesh of 236 elements with a refinement growing towards the free edge are used. The results for composite laminates [90o/0o]s, [0o/90o]s, [45o/-45o]s, [30o/-60o]s, [60o/-30o]s, [15o/-75o]s, [75o/-15o]s are presented and compared with references [3,4,5]. The results obtained show that the interlaminar stresses are generally confined to a boundary region or layer near or at the free edge, and the interlaminar stress components can be singular at the intersection of the free edge with the interface between two distinct layers. Because of the stress state in this boundary region of laminate it is not a plane stress state; the classical laminate theory is inadmissible in this region. The conclusion is that metis displacement method provided very good results in the treatment of a difficult problem comprising a singularity. The accuracy of the current solution is supported by some independent studies. It appears that the metis method provides a new method to calculate the interlaminar stresses in the free edge problem of composite laminates. References
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