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lenticular cross-section, and macroscopically homogeneous in-plane extension and
shear and transverse shear loadings are considered.
A unified prediction method ranging from micro model (named as fibre bundle
model) to macro model (named as weaving structure model) was developed by Fujita et
ai. (1995). In the fibre bundle model, one fibre bundle was modelled with beam
elements. Resin elements are set up to connect fibre beam elements. As the rule of
mixture is used to calculate the material constants of the fibre element, this model can
be used to study micro phenomena within fibre bundle. For the weaving structure
model, the weaving structure of textile composites is modelled by connecting the beam
elements. Resin existing between crossing fibre bundles is also modelled by resin
elements. The section of the fibre bundle is approximately in a rectangular shape,
whose area is assumed to be equal to that of the fibre bundle measured. This model was
only used to simulate the mechanical behaviours of 2D textile composites, and
dependence of the mechanical properties on the textile structural parameters was
however not investigated.
4.4 MODELS FOR 3D WOVEN COMPOSITES
In this section, we discuss several modelling schemes for typical 3D woven composites
as shown in Figure 4.12. There exist a variety of modelling schemes available.
However, our focus will be on the following selected three modelling schemes:
orientation averaging models, mixed iso-stress and iso-strain models, and finite element
applications.
(c)
Figure 4.12 Types of 3D woven fabrics, (a) 3D orthogonal interlock, (b) 3D Through-
thickness angle interlock, and (c) Layer-to-layer interlock (Tan, 1999)