Physics Technology Update (4th Edition)

Published by Pearson
ISBN 10: 0-32190-308-0
ISBN 13: 978-0-32190-308-2

Chapter 11 - Rotational Dynamics and Static Equilibrium - Problems and Conceptual Exercises - Page 367: 15

Answer

(a) $11N.m$ (b) $12N.m$ (c) $23N.m$

Work Step by Step

(a) The torque about the x-axis can be determined as follows: $I_x=m_1r_1^2+m_2r_2^2+m_3r_3^2$ $I_x=(9.0)(1.0)^2+0+0$ $I_x=9.0Kg.m^2$ Now $\tau_x=I_x\alpha$ We plug in the known values to obtain: $\tau_x=(9.0Kg.m^2)(1.20rad/s^2)$ $\tau_x=11N.m$ (b) The torque about the y axis can be determined as $I_y=0+0+(2.5)(2.0)^2=10Kgm^2$ Now$\tau_y=I_y\alpha$ We plug in the known values to obtain: $\tau=(10)(1.20)$ $\tau=12N.m$ (c) The torque about the z axis can be determined as follows: $I_z=(9.0)(1.0)^2+0+(2.5)(2.0)^2=19Kg.m^2$ Now $\tau_z=I_z\alpha$ $\implies \tau_z=(19Kg.m^2)(1.20rad/s^2)=23N.m$
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