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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 />

87

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