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Dynamics of Machines - Part II - IFS.pdf

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||y 1 (ω)|| [m/N]<br />

Phase [ o]<br />

Excitation on Point 2 and Response <strong>of</strong> Point 1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

−100<br />

−150<br />

−200<br />

−250<br />

−300<br />

0<br />

0 2 4<br />

Frequency [Hz]<br />

6 8<br />

0<br />

−50<br />

−350<br />

0 2 4<br />

Frequency [Hz]<br />

6 8<br />

||y 2 (ω)|| [m/N]<br />

Phase [ o]<br />

Excitation on Point 2 and Response <strong>of</strong> Point 2<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

−100<br />

−150<br />

−200<br />

−250<br />

−300<br />

0<br />

0 2 4<br />

Frequency [Hz]<br />

6 8<br />

0<br />

−50<br />

−350<br />

0 2 4<br />

Frequency [Hz]<br />

6 8<br />

Figure 27: Forced Vibration – Theoretical Frequency Response Function (FRF) <strong>of</strong> the clampedfree<br />

flexible beam when two concentrated masses m = m1 + m2 = 0.382 Kg are attached at its<br />

free end (L = 0.610 m) and two additional masses m = m1 + m2 = 0.382 Kg are attached at its<br />

middle (L = 0.310 m) – Natural frequencies <strong>of</strong> the 2. D.O.F. mass-spring system ”A”: 0.81 Hz<br />

and 5.56 Hz.<br />

44

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