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Páginas: 108 (26946 palabras) Publicado: 9 de junio de 2012
Problem 21.1 In Active Example 21.1, suppose that the pulley has radius R = 100 mm and its moment of inertia is I = 0.005 kg-m2 . The mass m = 2 kg, and the spring constant is k = 200 N/m. If the mass is displaced downward from its equilibrium position and released, what are the period and frequency of the resulting vibration?
k

R

Solution: From Active Example 21.1 we have
ω= k I m+ 2 R =(200 N/m) (2 kg) + (0.005 kg-m2 ) (0.1 m)2 = 8.94 rad/s

m

Thus τ= 2π 2π = = 0.702 s, ω 8.94 rad/s f = 1.42 Hz. f = 1 = 1.42 Hz. τ

τ = 0.702 s,

Problem 21.2 In Active Example 21.1, suppose that the pulley has radius R = 4 cm and its moment of inertia is I = 0.06 kg-m 2. The suspended object weighs 5 N, and the spring constant is k = 10 N/m. The system is initially at rest in itsequilibrium position. At t = 0, the suspended object is given a downward velocity of 1 m/s. Determine the position of the suspended object relative to its equilibrium position as a function of time.
k

R

m

Solution: From Active Example 21.1 we have
ω= k m+ I R2 = (10 N/m) 5N 9.81 m/s2 + (0.06 kg-m 2 ) (0.04 m) 2 = 0.51 rad/s

The general solution is x = A sin ωt + B cos ωt, v = Aω cos ωt −Bω sin ωt.

Putting in the initial conditions, we have x(t = 0) = B = 0 ⇒ B = 0, v(t = 0) = Aω = (1 ft/s) ⇒ A = Thus the equation is x = 1.96 sin 0.51t (m ). 1 m/s = 1.96 m . 0.51 rad/s

c 2008 Pearson Education South Asia Pte Ltd. All rights reserved. This publication is protected by Copyright and permission should be obtained from the publisher prior to any prohibited reproduction, storage ina retrieval system, or transmission in any form or by any means, electronic, mechanical, photocopying, recording or likewise.

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Problem 21.3 The mass m = 4 kg. The spring is unstretched when x = 0. The period of vibration of the mass is measured and determined to be 0.5 s. The mass is displaced to the position x = 0.1 m and released from rest at t = 0. Determine its position at t = 0.4 s.x k m

Solution: Knowing the period, we can find the natural frequency
ω= The general solution is x = A sin ωt + B cos ωt, v = Aω cos ωt − Bω sin ωt. 2π 2π = = 12.6 rad/s. τ 0.5 s

Putting in the initial conditions, we have x(t = 0) = B = 0.1 m ⇒ B = 0.1 m, v(t = 0) = Aω = 0 ⇒ A = 0. Thus the equation is x = (0.1 m) cos(12.6 rad/s t) At the time t = 0.4 s, we find x = 0.0309 m.

Problem21.4 The mass m = 4 kg. The spring is unstretched when x = 0. The frequency of vibration of the mass is measured and determined to be 6 Hz. The mass is displaced to the position x = 0.1 m and given a velocity dx/dt = 5 m/s at t = 0. Determine the amplitude of the resulting vibration.

x k m

Solution: Knowing the frequency, we can find the natural frequency ω = 2πf = 2π(6 Hz) = 37.7 rad/s. Thegeneral solution is x = A sin ωt + B cos ωt, v = Aω cos ωt − Bω sin ωt.

Putting in the initial conditions, we have x(t = 0) = B = 0.1 m ⇒ B = 0.1 m, v(t = 0) = Aω = 5 m/s ⇒ A = 5 m/s = 0.133 m. 37.7 rad/s

The amplitude of the motion is given by A2 + B 2 = (0.1 m)2 + (0.133 m)2 = 0.166 m.

Amplitude = 0.166 m.

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c 2008 Pearson Education South Asia Pte Ltd. All rights reserved. Thispublication is protected by Copyright and permission should be obtained from the publisher prior to any prohibited reproduction, storage in a retrieval system, or transmission in any form or by any means, electronic, mechanical, photocopying, recording or likewise.

Problem 21.5 The mass m = 4 kg and the spring constant is k = 64 N/m. For vibration of the spring-mass oscillator relative to itsequilibrium position, determine (a) the frequency in Hz and (b) the period.
k x

Solution: Since the vibration is around the equilibrium position,
we have k = m 1 cycle 64 N/m = 4 rad/s 4 kg 2π rad

m
20

(a)

ω=

= 0.637 Hz

(b)

τ =

2π 2π = = 1.57 s ω 4 rad/s

Problem 21.6 The mass m = 4 kg and the spring constant is k = 64 N/m. The spring is unstretched when x = 0. At t...
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