Abstract
An approximate method is presented to investigate the interlaminar stresses near the free edges of composite laminate plates that are subjected to a combined thermo-mechanical loading. The method is based upon admissible function representations of stresses which account for the effects of both the global mismatches and the local mismatches in two of the elastic properties, the Poisson's ratio and the coefficient of mutual influence. For this purpose, new thermo-mechanical mismatch terms are defined to reflect an effective deformation under the combined thermo-mechanical loading. Closed form solutions of all the stress components are sought by minimizing the complementary energy with respect to the unknown functions, in the stress representations, of the width coordinate. These unknown functions are determined by solving five ordinary differential equations along with a set of free edge boundary conditions, which allow complex as well as real roots for their exponential decaying rates. The resulting solutions satisfy the stress equilibrium and all of the boundary conditions exactly, but compatibility is met in a weak form. Numerical examples are given for several typical laminates, and are compared with previous results obtained by finite element and other approximate methods. It is found that the present approximate method yields interlaminar stress results in an efficient, fast and yet reliable way. It is also concluded that unlike some previous approximate methods, the current method is numerically robust and stable.
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Abbreviations
- A, B, D :
-
Laminate stiffness matrices as defined by (27)
- b :
-
Half laminate width
- ΔT (k) :
-
Temperature difference at the top of the k-th ply
- ΔT (k)(x 3):
-
Temperature difference in the k-th ply given as a function of through-thickness coordinate x 3
- e (k)0,1,2,3,12 :
-
Thermal strains of the k-th ply in the laminate axes
- h :
-
Laminate thickness
- M 11 :
-
Applied uniform bending load (moment/unit length)
- M Tij :
-
Applied thermal moments (moment/unit length)
- N :
-
Total number of plies
- N 11 :
-
Applied thermal loads (force/unit length)
- N Tij :
-
Applied thermal loads (force/unit length)
- Q (k)ij :
-
Ply stiffness for the k-th ply in the laminate axes
- S (k)ij :
-
Ply compliance for the k-th ply in the laminate axes
- t (k) :
-
Thickness of the k-th ply
- (x 1, x 2, x 3):
-
Local coordinate system with the out-of-plane coordinate x 3 defined at the bottom of each ply
- (x 1, x 2, z):
-
Global coordinate system with the out-of-plane coordinate z defined at the mid-plane of the laminate
- z (k) :
-
Global out-of-plane coordinate for the top of the k-th ply
- ε mech11 :
-
Applied mechanical axial strain
- ε tot11 :
-
Applied total (including thermal) axial strain
- εtot :
-
Total in-plane strain vector at arbitrary plane as defined by (32)
- ε0 :
-
Total in-plane strain vector at the midplane
- η12,1 :
-
Laminate coefficient of mutual influence
- η (k)12,1 :
-
Coefficient of mutual influence for the k-th ply
- η (k)12, 1E :
-
Equivalent coefficient of mutual influence for the k-th ply as defined by (23)
- K :
-
Total curvature vector
- μα,β,z :
-
Coefficients of thermal expansion for a uni-ply in its material principal axes
- μ (k)11,22,12,33 :
-
Coefficients of thermal expansion for the k-th ply in the laminate axes
- V12 :
-
Laminate Poisson's ratio
- ν (k)12 :
-
Poisson's ratio for the k-th ply
- ν (k)12E :
-
Equivalent Poisson's ratio for the k-th ply as defined by (22)
- σ i j :
-
Total stress components in tensor notation
- \(\widetilde\sigma _{ij} \) :
-
Far-field stress components
- σ c ij :
-
Companion stress components
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Communicated by S. N. Atluri, 30 August 1994
This work was supported by a grant from the Federal Aviation Administration, to the Center of Excellence for Computational Modeling of Aircraft Structures at Georgia Institute of Technology.
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Kim, T., Atluri, S.N. Analysis of edge stresses in composite laminates under combined thermo-mechanical loading, using a complementary energy approach. Computational Mechanics 16, 83–97 (1995). https://doi.org/10.1007/BF00365862
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DOI: https://doi.org/10.1007/BF00365862