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Composite Materials Research Progress

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<strong>Research</strong> Directions in the Fatigue Testing of Polymer <strong>Composite</strong>s 231<br />

Again there is a rigid-body constraint on all the partitions that do not make contact with<br />

the specimen, in order to save calculation time (Figure 29, left and right). The part is meshed<br />

with C3D8R elements; the element size is also 0.5 mm. The latter is done to assure that the<br />

calculation does not diverge as a result of contact problems.<br />

Figure 30 shows the final model of the fully-reversed three-point bending set-up.<br />

For the boundary conditions of the rotating support, only the rotation of the support<br />

around its ‘natural axis’ is allowed, all other movement is constrained.<br />

For the contact conditions, the slave surface is put on the support and the master surface<br />

is on the specimen. The latter helps the rotating of the support, since normally, the slave<br />

surface follows the movement of the master surface.<br />

The specimen is a beam with dimensions 2.4 mm x 15 mm x 80 mm and it is meshed<br />

with quadratic brick elements with reduced integration, C3D20R. The global size of the<br />

elements is 3 mm. However, in the zones of contact, the size is 1 mm to ensure that no<br />

convergence problems occur due to the contact conditions. The material model is the same<br />

linear elastic model as in paragraph 4.1 (see Table 1).<br />

Figure 30. Illustration of the mesh and the boundary conditions for the three-point bending setup with<br />

rotating supports [47].<br />

With this model, the bending stresses in the experimental fatigue tests could be simulated<br />

very well. More details can be found in [47].<br />

4.4. Cantilever Bending Fatigue<br />

This paragraph deals with the correct modelling of the set-up for cantilever bending fatigue<br />

that was already shown in Figure 7. It is tempting to model the clamped side of the specimen<br />

by a number of fully constraint nodes in the finite element mesh. However, this model<br />

appears to add unwanted stiffness to the specimen and the predicted force is considerably<br />

higher than the measured one.<br />

The calculations were done for a plain weave glass/epoxy specimen. The prescribed<br />

displacement umax (= 34.4 mm) was chosen rather large in order to assess the effect of<br />

geometrical non-linearities. The corresponding maximum bending force for the specimen,

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