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Civil-Comp Proceedings
ISSN 1759-3433 CCP: 75
PROCEEDINGS OF THE SIXTH INTERNATIONAL CONFERENCE ON COMPUTATIONAL STRUCTURES TECHNOLOGY Edited by: B.H.V. Topping and Z. Bittnar
Paper 82
A C1 Triangular Finite Element for Analyzing Multilayered Shell Structures F. Dau+, O. Polit* and M. Touratier+
+LMSP, ENSAM, Paris, France
F. Dau, O. Polit, M. Touratier, "A C1 Triangular Finite Element for Analyzing Multilayered Shell Structures", in B.H.V. Topping, Z. Bittnar, (Editors), "Proceedings of the Sixth International Conference on Computational Structures Technology", Civil-Comp Press, Stirlingshire, UK, Paper 82, 2002. doi:10.4203/ccp.75.82
Keywords: finite element, refined shell model, multilayered structures,.
Summary
The aim of this work is to analyze the mechanical behaviour of multilayered
structures by shell finite element including transverse shear effects and
continuity requirements between layers in order to predict displacements
and stresses of such composite structures for design applications.
Based on a conform finite element method, a new C1 triangular six
node finite element is presented.
This element is based on a refined kinematic model [1],
using only five generalized displacements, to
assure :
The displacement field for each elastic layer denoted of a laminated shallow shell is given by :
where are the two transverse shear strain components at the middle surface of the shell () and . In this expressions, we denote the in-surface displacements, the transverse displacement and the two rotations. In addition, are trigonometric functions of and are linear functions of determined from the boundary conditions on the top and bottom surfaces of the shell, and from the continuity requirements at the layer interfaces for displacements and stresses, see Reference [1]. Several strain models, called Complete model, Love model and Love-Donnell model are deduced from the displacement field according to appropriate assumptions such as (i.e where denotes curvature tensor) due to geometry or/and neglecting membrane coupling in transverse shear expression, ... Concerning the geometry of the shell, this one is described with an explicit map between curvilinear co-ordinates associated with the middle surface of the shell and cartesian co-ordinates. The main interest is to calculate analytically all the geometric characteristics of the shell : local covariant basis, metric and curvature tensors, Christoffel symbols, ...are needed. The generalized displacements and are approximated by higher-order polynomia [2] based on :
This permits to ensure a conform finite element method and to avoid locking phenomenon. References
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