Consider the system in Figure 1-a, which is initially at equilibrium. The massless bar AOB with point mass m = 2 kg attached to B rotates with rotational viscous damping coefficient b about the fixed point O. The system is connected by a horizontal spring (acting at B) to a fixed wall. The rotating bar has a length 3L=1.5 meters. L 2L k 17 win A Rotational viscous damping coefficient b B g Massless
Consider the system in Figure 1-a, which is initially at equilibrium. The massless bar AOB with point mass m = 2 kg attached to B rotates with rotational viscous damping coefficient b about the fixed point O. The system is connected by a horizontal spring (acting at B) to a fixed wall. The rotating bar has a length 3L=1.5 meters. L 2L k 17 win A Rotational viscous damping coefficient b B g Massless
Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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
Transcribed Image Text:Consider the system in Figure 1-a, which is initially at equilibrium. The massless bar AOB with point mass
m = 2 kg attached to B rotates with rotational viscous damping coefficient b about the fixed point
system is connected by a horizontal spring (acting at B) to a fixed wall. The rotating bar has a length 3L=1.5
meters.
L
2L
k
twine
ww
Figure 1-a
A
Rotational viscous
damping coefficient b
B
g
Massless
a) Write the linearized equation of motion of the system (Figure 1-a) for small angular displacement 0 (t).
(Symbolic)
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