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2023 | OriginalPaper | Chapter

2. Classical Laminate Theory

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Abstract

This chapter first covers the mechanical modeling of a single layer with unidirectionally aligned reinforcing fibers embedded in a homogeneous matrix, a so-called lamina. It is shown that a lamina can be treated as a combination of a plane elasticity element and a classical plate element. For both classical structural elements and their combination, the continuum mechanical modeling based on the three basic equations, i.e., the kinematics relationship, the constitutive law, and the equilibrium equation is presented. Combining these three questions results in the governing partial differential equations. The second part of the chapter covers the stacking of single laminae, generally under different angles, to a so-called laminate. Based on the approach of the classical laminate theory, a simplified stress analysis, and a subsequent failure analysis is derived, without the solution of the system of coupled differential equations for the unknown displacements in the three coordinate directions. This theory provides the solution of the statically indeterminate system based on a generalized stress-strain relationship under consideration of the constitutive relationship and the definition of the so-called stress resultants.

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Footnotes
1
Note that according to the assumptions of the classical thin plate theory, the lengths \(\overline{\textit{0A}}\) and \(\overline{\textit{0}'{} \textit{A}'}\) remain unchanged.
 
2
Three-dimensional isotropy requires as well only two independent elastic constants.
 
3
Three-dimensional orthotropy requires nine independent elastic constants.
 
4
In the case of a shear force \(\sigma _{ij}\), the first index i indicates that the stress acts on a plane normal to the i-axis and the second index j denotes the direction in which the stress acts.
 
5
If gravity is acting, the body force f results as the product of density times standard gravity: \(f=\tfrac{F}{V}=\tfrac{mg}{V}=\tfrac{m}{V}g=\varrho g\). The units can be checked by consideration of \(1\,\text {N}=1\tfrac{\text {m}\text {kg}}{\text {s}^2}\).
 
6
Thus, symmetric angle-ply laminates do not belong to the group of symmetric balanced laminates.
 
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Metadata
Title
Classical Laminate Theory
Authors
Andreas Öchsner
Resam Makvandi
Copyright Year
2023
DOI
https://doi.org/10.1007/978-3-031-32975-3_2

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