Master Thesis - OUFTI-1
Master Thesis - OUFTI-1
Master Thesis - OUFTI-1
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In our case, only the SMT and heavy components will be included in the FE model of<br />
the OBC 2 card. The light components, due to their negligible eect on the stiness and<br />
mass properties of the PCB, will not be modeled in any application. The Catia modeling<br />
of the OBC 2 card is presented in Figure 4.13.<br />
Figure 4.13: Catia modeling of the OBC 2 card<br />
To take into account the mass contributions of these components on the OBC 2 response,<br />
the methods exposed in section 4.2.5 will be applied one by one. Thus, the accuracy<br />
of each of them will be discussed, based on experimental results obtained through the<br />
test that will be presented in section 4.3.3.<br />
The stiness contributions will not be included in FE models for several reasons:<br />
• First, the datasheets provided with most electronic components, do not contain this<br />
information.<br />
• Then, realizing a static bend test on each component is too expensive with regard to<br />
the expected results.<br />
• Finally, as already mentioned, ignoring the stiness is a conservative approach. So,<br />
the natural frequencies that will be obtained, will be lower than the real ones. This<br />
fact is not critical in our case because, in general, LV manuals specify minimum<br />
values for the payload natural (fundamental) frequency of vibration in order to avoid<br />
dynamic coupling between low frequency dynamics of the LV and payload modes.<br />
So, if the natural frequencies obtained using this method fulll the requirements, the<br />
real ones will automatically fulll these requirements. An example of this type of<br />
requirement is presented in Figure 4.14.<br />
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