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 371: 84

Answer

(a) $15.8Nm$ (b) greater (c) $2560rpm$

Work Step by Step

(a) We can find the required torque as follows: $\tau=I\alpha$ $\implies \tau=(\frac{1}{2}mr^2)(\frac{\omega^2}{2\Delta \theta})$ $\implies \tau=\frac{1}{4}(\frac{mr^2\omega^2}{\Delta \theta})$ We plug in the known values to obtain: $\tau=\frac{1}{4}\frac{(0.755Kg)(0.152m)^2(362\pi/3 rad/s)^2}{12.6\pi rad}$ $\tau=15.8Nm$ (b) We know that the angular speed of the saw blade is directly proportional to the square root of the angular displacement; thus, it will be greater than 1810 rpm. (c) We can find the required angular speed as follows: $\omega=\sqrt{\frac{4\tau \Delta \theta}{mr^2}}$ We plug in the known values to obtain: $\omega=\sqrt{\frac{4(15.8Nm)(6.30\pi rad)}{(0.755Kg)(0.152m)^2}}$ $\omega=2560rpm$
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