The measurement bandwidth was increased so that the first three modes were captured. Again, the direct, (X_{1}

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The measurement bandwidth was increased so that the first three modes were captured. Again, the direct, \(X_{1} / F_{1}\), and cross FRFs, \(X_{2} / F_{1}\) through \(X_{5} / F_{1}\), were measured. The imaginary part of the direct FRF for the entire bandwidth is shown in Fig. P6.6a. The three natural frequencies are 200, 550, and 1,250 Hz.

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Fig. P6.6a Direct FRF \(X_{1} / F_{1}\).
Use Figs. P6.6b through P6.6f to identify the mode shape that corresponds to the \(1,250 \mathrm{~Hz}\) natural frequency. Plot your results using the same approach described.

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Fig. P6.6b Direct \(\mathrm{FRF} X_{1} / F_{1}\) (mode 3 only).

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Fig. P6.6c Cross FRF \(X_{2} / F_{1}\).

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Fig. P6.6d Cross FRF \(X_{3} / F_{1}\).

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Fig. P6.6e Cross FRF \(X_{4} / F_{1}\).

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Fig. P6.6f Cross FRF \(X_{5} / F_{1}\).


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Mechanical Vibrations Modeling And Measurement

ISBN: 119669

1st Edition

Authors: Tony L. Schmitz , K. Scott Smith

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