Dynamics of Machines - Part II - IFS.pdf
Dynamics of Machines - Part II - IFS.pdf
Dynamics of Machines - Part II - IFS.pdf
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1.7.9 Resonance – Experimental Analysis in Time Domain<br />
(a) Amplitude [m/s 2 ]<br />
1<br />
0<br />
−1<br />
x Signal 10−5<br />
2<br />
(a) in Time Domain − (b) in Frequency Domain<br />
−2<br />
0 5 10 15<br />
time [s]<br />
20 25 30<br />
(b) Amplitude [m/s 2 ]<br />
4<br />
3<br />
2<br />
1<br />
x 10 −6<br />
0<br />
0 5 10 15 20 25<br />
frequency [Hz]<br />
(a) Amplitude [m/s 2 ]<br />
1<br />
0<br />
−1<br />
x Signal 10−5<br />
2<br />
(a) in Time Domain − (b) in Frequency Domain<br />
−2<br />
0 5 10 15<br />
time [s]<br />
20 25 30<br />
(b) Amplitude [m/s 2 ]<br />
8<br />
6<br />
4<br />
2<br />
x 10 −6<br />
0<br />
0 5 10 15 20 25<br />
frequency [Hz]<br />
Figure 31: Resonance phenomena due to the excitation force with frequency around the natural<br />
frequency <strong>of</strong> the mass-spring system: 2 D.O.F. system with the natural frequencies <strong>of</strong> 0.62 Hz<br />
and 4.59, excited by the shaker – Spring-mass system ”A” with three masses m = m1+m2+m3 =<br />
0.573 Kg fixed at the beam length L2 = 0.610 m and three additional masses m = m4+m5+m6 =<br />
0.573 Kg fixed at the middle L1 = 0.310 m resulting in two natural frequencies <strong>of</strong> 0.62 Hz and<br />
4.60 Hz.<br />
48