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Fig. 5.11 Load and boundary conditions in the case of the curved layer FDM part<br />

5.6 Results and discussion<br />

A lot of data is generated from the finite element analysis of the stress fields of the<br />

two parts in terms of displacements and various stress components. However, the<br />

finite element results are mainly considered to compare the maximum displacement<br />

values with the maximum allowable displacement of the material as generated by the<br />

tensile test conducted on the raw material and presented in the load-displacement<br />

diagram of Fig. 5.6. The reason for this is a lack of experimental data on other<br />

parameters. The distribution of the stress components will also be used, but mainly<br />

to assess the stress patterns generated in different material deposition schemes.<br />

Each of the model is analysed for a time dependent variation of the applied loads.<br />

Fig. 5.12 presents a series of screen shots showing the gradual increase in the<br />

applied load and the corresponding variation in the displacement. There is a peculiar<br />

problem observed in the case of the flat layer FDM model, the applied load is<br />

concentrated at a few points, in a very narrow zone. The component assumes a<br />

completely distorted shape, and to reach the target load of 400-500 N overall, it was<br />

necessary to increase the total of nodal loads beyond 900 N. The model was tested<br />

a number of times, with all load and boundary conditions repeatedly checked, but the<br />

end result was the same. It was finally concluded that the relatively weak interaction<br />

between the flat layers, in particular at regions, where the part bends into a curved<br />

shape from the flat portions leads to an early failure and the strands are almost<br />

115

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