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 676: 62

Answer

$x=\frac{mr\omega_{\circ}^2L^3}{48EI-M\omega_{\circ}^2L^3}$

Work Step by Step

The required amplitude can be determined as follows: $K=\frac{P}{\delta}$ $\implies K=\frac{P}{\frac{PL^3}{48EI}}$ $\implies K=\frac{48EI}{L^3}$ We know that $\omega_n=\frac{K}{m}$ $\omega_n=\frac{48EI/L^3}{M}$ $\implies \omega_n=\frac{48EI}{ML^3}$ As $F_{\circ}=mr\omega_{\circ}^2$ Now $x=|\frac{F_{\circ}/K}{1-(\frac{\omega_{\circ}}{\omega_n})^2}|$ $\implies x=\frac{\frac{m\omega_{\circ}^2r}{48EI/L^3}}{1-(\frac{\omega_{\circ}}{\sqrt{\frac{48EI}{ML^3}}})^2}$ This simplifies to: $x=\frac{mr\omega_{\circ}^2L^3}{48EI-M\omega_{\circ}^2L^3}$
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