36th Structures, Structural Dynamics and Materials Conference 1995
DOI: 10.2514/6.1995-1211
|View full text |Cite
|
Sign up to set email alerts
|

An efficient thick beam theory and finite element model with zig-zag sublaminate approximations

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
16
0

Year Published

1996
1996
2015
2015

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 14 publications
(16 citation statements)
references
References 5 publications
0
16
0
Order By: Relevance
“…Since TOT has the same number of displacement variables as the present theory and does not require an arbitrary shear correction factor, results are also compared with the coupled TOT [16]. Simply [25,31] are considered: The frequencies ω n and the modal entities are non-dimensionalised as follows with S = a/ h:…”
Section: Results and Assessmentmentioning
confidence: 99%
“…Since TOT has the same number of displacement variables as the present theory and does not require an arbitrary shear correction factor, results are also compared with the coupled TOT [16]. Simply [25,31] are considered: The frequencies ω n and the modal entities are non-dimensionalised as follows with S = a/ h:…”
Section: Results and Assessmentmentioning
confidence: 99%
“…The stacking order is mentioned from the bottom. The five-ply substrate of beam (a) is a good test case, [21]. It has plys of thickness 0:09h=0:225h=0:135h=0:18h=0:27h of materials 1=2=3=1=3 which have highly inhomogeneous stiffness in tension and shear.…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…The reference plane z ¼ 0 either passes through or is the bottom surface of the k 0 -th layer. For a beam with small width, the usual assumptions for mathematical simplification of 1D model made by other researchers, [8,15,21], which are retained in the present theory, are: assume plane state of stress ðr y ¼ s yz ¼ s xy ¼ 0Þ, neglect transverse normal stress ðr z ' 0Þ and assume the axial and transverse displacements u; w and electric potential / to be independent of y ð) electric field component E y ¼ À/ ;y ¼ 0Þ. The strain-displacement and electric field-potential relations for directions x; z are where a subscript comma denotes differentiation.…”
Section: Formulation Of Layerwise Statical Theorymentioning
confidence: 99%
“…They are a drawback since they prevent the formulation of C 0 computationally efficient finite elements. The C 1 continuity requirement of conventional ZZ models that does not exhibit a piecewise variation of the transverse displacement has been circumvented by Averill [33] and Averill and Yip [34] using interdependent interpolation (see, Tessler and Dong [51]) and penalty function concepts (see, Reddy [53]). In this paper, the following representation is introduced to convert first-order derivatives into new variables:…”
Section: Displacement and Stress Fieldsmentioning
confidence: 99%