Engineering Mechanics: Statics & Dynamics (14th Edition)

Published by Pearson
ISBN 10: 0133915425
ISBN 13: 978-0-13391-542-6

Chapter 22 - Vibrations - Section 22.6 - Electrical Circuit Analogs - Problems - Page 674: 44

Answer

$$ y=(-3.66 \sin 12.25 t+50 \cos 12.25 t+11.2 \sin 4 t) \mathrm{mm} $$

Work Step by Step

$$ \omega_h=\sqrt{\frac{k}{m}}=\sqrt{\frac{600}{4}}=12.25 $$ The general solution is defined by Eq. $22-23$ with $k \delta_0$ substituted for $F_0$. $$ y=A \sin \omega_n t+B \cos \omega_n t+\left(\frac{\delta_0}{\left[1-\left(\frac{\omega}{\omega_n}\right)^2\right]}\right) \sin \omega t $$ $\delta=(0.01 \sin 4 t) \mathrm{m}$, hence $\delta_0=0.01, \omega=4$, so that $y=A \sin 12.25 t+B \cos 12.25 t+0.0112 \sin 4 t$ $y=0.05$ when $t=0$ $0.05=0+B+0 ; \quad B=0.05 \mathrm{~m}$ $\dot{y}=A(12.25) \cos 12.25 t-B(12.25) \sin 12.25 t+0.0112(4) \cos 4 t$ $v=y=0$ when $t=0$ $0=A(12.25)-0+0.0112(4) ; \quad A=-0.00366 \mathrm{~m}$ Expressing the result in mm, we have $y=(-3.66 \sin 12.25 t+50 \cos 12.25 t+11.2 \sin 4 t) \mathrm{mm}$
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