posted on 2022-11-17, 14:52authored byLisa M.A. Cahill
The standard Finite Element Method (FEM) has been successfully employed for many decades in
modelling. However, the method can be found, in cases, to be insufficient for accurate, efficient
modelling of discontinuities, such as those inherently present within the morphology of composite
materials and those induced in the fracture of these materials.
This thesis develops state-of-the-art approaches to quantify meso-scale cracking within composite
laminae. Both experimental and numerical techniques are employed and the findings of this
research will aid the development of more damage tolerant approaches when designing with composite
materials. The eXtended Finite Element Method (X-FEM) is used to develop a numerical
model, sufficient to simulate crack growth in a typical aerospace composite, at lamina level. The
XFE model developed herein is extended to analyse the interactions of multiple cracks within a
carbon fibre epoxy lamina, represented as an orthotropic material. It is initially confirmed that,
similar to isotropic materials, collinear cracks amplify the mode I stress intensity factor (KI). In
contrast, parallel cracks are found to shield, and hence, reduce the KI value upon approach. However,
the fibre orientation plays a far more significant role when cracks are configured ‘offset’ to
each other. It is found that crack tips sharing a fibre orientation will significantly amplify KI . This
phenomenon is also evident in studies featuring arrays of cracks. The insight gained from this
study should better guide design when known stress raisers are to be included in composite structures.
Notwithstanding this, it was found, both numerically and experimentally, that cracks do
not interact on propagation, the crack trajectory is at all times controlled by the fibre orientation.
Numerically, orthotropic strips, assumed to be perfectly bonded, were studied. The configuration
of the material orientations was also found to affect the stress intensity. The crack trajectory however,
remained controlled by the fibre orientation.
Two bespoke experimental test series have confirmed the XFE model predictions for both loaddisplacement
and the crack propagation direction. The test series have also allowed, in conjunction
with the XFEmodel, fracture toughness values (KIc) to be calculated. The variation in fracture
toughness, with changing fibre orientation, has been fitted by a hyperbolic function. This allows
prediction of fracture toughness values, for a range of material orientations, knowing only the
fracture toughness for the 0◦ lamina. The effect of crack geometry and configuration on fracture
toughness is also addressed in detail.
Acomplete methodology for calculation of fracture toughness values from images acquired during
the experimental testing is finally presented. The method relies on using digital image correlation
to extract the displacement field about the crack tip, hence requiring high quality image acquisition.
The combined experimental-numerical approach makes use of an interaction integral with
the experimental displacement field to obtain KIc values. The method provides a simple yet robust
technique for extraction of fracture parameters from non-standard test specimens.