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Dynamics of Machines - Part II - IFS.pdf

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(a) Amplitude [m/s 2 ]<br />

(b) Amplitude [m/s 2 ]<br />

(a) Amplitude [m/s 2 ]<br />

(b) Amplitude [m/s 2 ]<br />

(a) Amplitude [m/s 2 ]<br />

(b) Amplitude [m/s 2 ]<br />

2<br />

1<br />

0<br />

−1<br />

−2<br />

x 10 −5 Signal (a) in Time Domain − (b) in Frequency Domain<br />

0 5 10 15<br />

time [s]<br />

20 25 30<br />

1.5<br />

1<br />

0.5<br />

x 10 −5<br />

0<br />

0 5 10 15 20 25<br />

frequency [Hz]<br />

2<br />

1<br />

0<br />

−1<br />

−2<br />

1.5<br />

0.5<br />

x 10 −5 Signal (a) in Time Domain − (b) in Frequency Domain<br />

0 5 10 15<br />

time [s]<br />

20 25 30<br />

1<br />

x 10 −5<br />

0<br />

0 5 10 15 20 25<br />

frequency [Hz]<br />

2<br />

1<br />

0<br />

−1<br />

−2<br />

1.5<br />

0.5<br />

x 10 −5 Signal (a) in Time Domain − (b) in Frequency Domain<br />

0 5 10 15<br />

time [s]<br />

20 25 30<br />

1<br />

x 10 −5<br />

0<br />

0 5 10 15 20 25<br />

frequency [Hz]<br />

Figure 35: Resonance phenomena due to the excitation force with frequencies around the natural<br />

frequencies <strong>of</strong> the mass-spring system: 3 D.O.F. system with the natural frequencies <strong>of</strong> 0.75 Hz,<br />

5.12 Hz and 14.68 Hz, excited by the shaker – Spring-mass system ”A” with two masses m =<br />

m1 + m2 = 0.382 Kg fixed at the beam length L3 = 0.610 m, two additional masses fixed at<br />

L2 = 0.410 m and two more at L1 = 0.210 m.<br />

57

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