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Dynamics of Machines - Part II - IFS.pdf

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(a) y(t) [m]<br />

(b) y(t) [m]<br />

(c) y(t) [m]<br />

0.01<br />

0.005<br />

0<br />

−0.005<br />

(a) Exact Solution − (b) Numerical Solution (delta T = 0.01 s) − (c) Comparison<br />

−0.01<br />

0 1 2 3 4 5<br />

time [s]<br />

6 7 8 9 10<br />

0.01<br />

0.005<br />

0<br />

−0.005<br />

−0.01<br />

0 1 2 3 4 5<br />

time [s]<br />

6 7 8 9 10<br />

0.01<br />

0.005<br />

0<br />

−0.005<br />

−0.01<br />

0 1 2 3 4 5<br />

time [s]<br />

6 7 8 9 10<br />

Figure 9: Comparison between the analytical and numerical solutions when a time step <strong>of</strong> 0.01 [s]<br />

is used – Good agreement between the numerical and analytical solutions in the total range <strong>of</strong><br />

time.<br />

(a) y(t) [m]<br />

(b) y(t) [m]<br />

(c) y(t) [m]<br />

1<br />

0.5<br />

0<br />

−0.5<br />

(a) Exact Solution − (b) Numerical Solution (delta T = 0.01 s) − (c) Comparison<br />

−1<br />

0 5 10 15<br />

time [s]<br />

20 25 30<br />

1<br />

0.5<br />

0<br />

−0.5<br />

−1<br />

0 5 10 15<br />

time [s]<br />

20 25 30<br />

1<br />

0.5<br />

0<br />

−0.5<br />

−1<br />

0 5 10 15<br />

time [s]<br />

20 25 30<br />

Figure 10: Comparison between the analytical and numerical solutions when a time step <strong>of</strong><br />

0.01 [s] is used – Good agreement between the numerical and analytical solutions in the total<br />

range <strong>of</strong> time. System behavior when excited by a harmonic force with a frequency near the<br />

natural frequency.<br />

18

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