Simple Application of the Modified Finite Element Method Displacement Approach for Geometrical Nonlinear Analysis of Composite Plates
   Researchers
Abstract
Keywords
Introduction
Modified finite element
Finite element formulation
Linear stiffness matrix
Numerical results and discussion
Conclusions
Reference

 Ibraheem Hssn 
 Postgraduate student (PhD), Department of Structural Engineering, Faculty of civil engineering, Tishreen University, Lattakia, Syria
ibhassan@tishreen.edu.sy

Sulaiman Abo Diab
Associate Professor, Department of Structural Engineering, Faculty of civil engineering, Tishreen University, Lattakia, Syria
‫sabodiab@tishreen.edu.sy‬‬‬‬‬‬‬‬‬‬‬‬‬‬‬‬‬‬‬‬‬‬‬‬

Bassam Hwaija

Professor, Department of Structural Engineering, Faculty of civil engineering, Tishreen  University, Lattakia, Syria
h.bassam65@yahoo.com


 
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Abstract


A displacement-based modified finite element is applied in this paper to analyze multilayered composite plates in the geometrical nonlinear domain. The proposed plate element is based on the first-order shear deformation theory (FSDT) and von Karman's large deflection theory while the displacement approach is based on the incremental form of the principle of virtual displacement. The displacement function is modified and new terms have been added to consider the effect of the external load. As a result, shape functions are classified into two categories the first one is the homogenous shape functions relevant to degrees of freedom and the second is the nonhomogeneous shape functions related to the element loading. Lastly, some examples are computed and the results of displacements are compared with analytical/experimental and other numerical solutions available in the literature. Numerical examples showed that results from applying the present element were in good agreement with other solutions.



 

 
 Keywords: Displacement approach, FEM, Composite plates, Nonlinear analysis  
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 Introduction


Plates are very common elements used in all engineering fields such as transportation, aerospace and civil engineering. One of the most recent and currently used plates is the multilayered composite plates (Laminates), which are plates consists of number of layers placed over each other. In each layer we can use different materials also we can orient them in various directions. This structure of composite plates gives better engineering properties than ordinary plates with one material in one direction. Figure (1) shows a composite plate made of several layers of Carbon fibers connected with each other using Epoxy.

 
   
 Figure(1). Multilayered composite plate of Carbon fiber  
 Multilayered composite plates has been studied in nonlinear case by many researchers and using different methods (analytical and experimental) but due to mathematical difficulties in solving the differential equation governing the behavior of these plates, numerical methods were used as an alternative solution that provides acceptable approximate results. We aren't going to introduce a long historical background about multilayered composite plates in nonlinear domain but for readers who looking for more background you can see references [1,2] which are among first papers that studied this field. Also references [3-14] represents a sample of important papers that contributed significantly in the development of nonlinear analysis of multilayered composed plates.
First study : Zhang and Kim [15] studied thin to moderate thickness composite plates in geometrical nonlinear domain using finite element method displacement approach by implementing the principle of virtual displacement and applying incremental iterative approach (Newton-Raphson method). Results showed that the two proposed elements (RDKQ-NL20) and (RDKQ-NL24) give exact solutions without applying large number of steps or using a very soft mesh. Second study : Reddy and Arthur [16] studied multilayered composite plates in geometrical nonlinear domain using mixed finite element model. The proposed element has 8 degrees of freedom (3 displacement, 2 rotations and 3 bending moments). The researchers concluded that increasing the number of layers contributes to mitigating the nonlinear effect of the curvature with load increase.
The finite element displacement approach presented here, use displacement approximation basis. The parametric form chosen fulfils strictly the differential equation of the Kirchhoff’s plate. The free parameters are related to the degrees of freedoms of the element in an analogous way adopted in the conventional finite element displacement approach. As a result, the shape functions are separated into two parts, a homogenous part related to the degrees of freedom of the element and a new non-homogenous part dependent on the element loading at the finite element level
.

 
 
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 Modified finite element


In the modified finite element method, the shape functions supposed to achieve the differential equation accurately, but because of the difficulty of finding exact solutions for the von Karman equation which expresses the geometrical nonlinear behavior of plates and since we study the nonlinear behavior as a series of small linear steps we will use the shape functions of the standard 4 node quadrilateral isoparametric  plane element as the homogeneous part of shape functions.


N_1 (θ^1,θ^2 )=(1/4)(1-θ^1 )(1-θ^2 )      ;     N_2 (θ^1,θ^2 )=(1/4)(1+θ^1 )(1-θ^2 )                (1)
N_3 (θ^1,θ^2 )=(1/4)(1+θ^1 )(1+θ^2 )      ;     N_4 (θ^1,θ^2 )=(1/4)(1-θ^1 )(1+θ^2 )                (2)


For nonhomogeneous part we will consider the displacement function for ACM element and extend it to contain fifteen parameters instead of twelve then match both sides of the differential equation governing the behavior of plates in linear state. These steps are explained in detail in references [17-21].
In final form we will obtain the displacement function as follows :


w_i=N_i^m(e) .u_m(e) +N ̅_ij.p ̅^j                                (3)


N_i^m(e)  : Homogeneous part of shape functions, u_m(e)  : Nodal degrees of freedom.
N ̅_ij : Nonhomogeneous part of shape functions which given in detail in [21] .
p ̅^j : Distributed load intensity at the nodal points of the element.


 

 Finite element formulation

 

 
 By applying the incremental form of the principle of the virtual displacement and take it as the variational basis for finite element method displacement approach then we can consider the first variation of total energy is equivalent to zero  

 
δ∆π=0                                                                     (4)


Using incremental procedure to proceed from a given state of equilibrium to unknown state then the corresponding u_i^0 displacements are replaced by a new displacement u_i and the body moves to new position its displacement is u ̃_i :
u ̃_i=u_i^0+u_i                                                               (5)


u_i : Small increment in displacement.
σ_ij=σ_ij^0+〖∆σ〗_ij    ;   ε_ij=ε_ij^0+〖∆ε〗_ij                     (6)


ε_ij^0  ,σ_ij^0 : Strain and stress tensors.
〖∆ε〗_ij  ,〖∆σ〗_ij : Small increments in strain and stress respectively which resulted from the increment in displacement.
According to the principle of virtual displacement the variation of total energy is :

 
 
 
 
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Linear stiffness matrix

 

 
   
 

Linear bending stiffness matrix K_Eb
:
 
 
Bb : First order partial derivatives of homogeneous shape functions with respect to (x,y) respectively and they express the bending behavior of the plate.
Qb : Elasticity tensor which express the bending behavior for all layers
.
 
 
Shear stiffness matrix K_S   
 
 
 
 
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Numerical results and discussion


    Clamped square plate under uniformly distributed load
This example is widely considered as benchmark problem to check and verify geometrical nonlinear behavior of thin plate formulations [16]. Plate dimensions are (L=300in ,t=3in). Material properties, Young modulus in x and y directions : (E_1=E_2=30×〖10〗^6 Psi), Possion ratio (ϑ_12=ϑ_21=0.316)
The plate is subjected to uniform distributed load, the thickness of all individual layers within the plate are equal, shear correction factor is taken (5/6),  20 incremental load steps are applied and the convergence tolerance used here is(0.001). The results of the nondimensional central deflection (w/t) and nondimensional normal stress (σ_xx.t^2/L^2.q) from modified element, Reddy and Urthaler [16] and analytical solution [5] are presented in table 1.

 

 
 

The diagram of nondimensional central deflection (w/t) and normal stress (σ_xx.t^2/L^2.q) with nondimensional load (q.L^4/E_2.t^4 ) from modified element, Reddy and Urthaler [16] and analytical solution [5] are presented in figures 2 and 3
.
 
 
 
Figure(2). Relationship between nondimensional deflection (w/t) and nondimensional load ((q.L^4/E_2.t^4 )) at center of clamped square plate (L/t=100)  
 
Figure(3). Relationship between nondimensional normal stress (σ_xx.t^2/L^2.q) and nondimensional load (q.L^4/E_2.t^4 ) at center of clamped square plate (L/t=100)
    Simply supported 4 layer (0^°/〖90〗^°/〖90〗^°/0^° ) square plate

 
 
In this example we will study three cases in each case the ratio of plate length to thickness (L/t) is (10, 20, 40) respectively. The plate consists of four layers oriented (0^°/〖90〗^°/〖90〗^°/0^° ). Material properties satisfies the following relations :
(E_1/E_2=25  ;  G_12/E_2=0.5  ;  G_23/E_2=0.2  ;  G_12=G_13 ), Young modulus in x direction : (E_1=25×〖10〗^6 Psi), Young modulus in y direction : (E_2=〖10〗^6 Psi)
Shear modulus : (G_12=G_13=0.5×〖10〗^6 Psi) , (G_23=0.2×〖10〗^6 Psi) , Possion ratio (ϑ_12=ϑ_21=0.25), the plate is subjected to uniform distributed load (q=2Psi), the thickness of all individual layers are equal, shear correction factor is taken (5/6), 20 incremental load steps are applied and the convergence tolerance used here is(0.01). The results of the nondimensional central deflection (w/t) from modified element, Zhang and Kim [15] and analytical solution [4] for the three cases (L/t=10 ,20 ,40) are presented in table 2
.
 
 
 
 
 Figure(4). Relationship between nondimensional deflection (w/t) and nondimensional load (q.L^4/E_2.t^4 ) at center of simply supported square plate for various ratios (L/t=10,20,40) obtained from modified element  
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Conclusions


•    Modified method is able to deal with the incremental form of geometrical nonlinear analysis of multilayered composite plates, and even though it requires to use displacement functions satisfies the differential equation at the element level, it is possible to roughly use the solution of the differential equation for the linear case as an initial approximation to the nonlinear case.


•    The proposed modified element gave great convergence to the analytical solution, despite it can be considered simple in terms of mathematical formulation and compared to other proposed elements.


•   
For the practical applications (especially composite plates in aerospace) the method presented in this article give fast and easy initial results for displacements since the shape functions aren't complicated from mathematical point of view and the nonhomogeneous part takes into account the type of loading on the plate.


 

 
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References :


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