University Physics with Modern Physics (14th Edition)

Published by Pearson
ISBN 10: 0321973615
ISBN 13: 978-0-32197-361-0

Chapter 9 - Rotation of Rigid Bodies - Problems - Exercises - Page 294: 9.4

Answer

(a) $\alpha_z(t) = (-1.60~rad/s^3)~t$ (b) $\alpha_z = -4.80~rad/s^2$ $\alpha_{ave} = -2.40~rad/s^2$ The two quantities are different because the angular acceleration changes as a function of time. The angular acceleration is not constant.

Work Step by Step

(a) $\omega_z(t) = \gamma -\beta ~t^2$ $\alpha_z(t) = \frac{d\omega}{dt} = -2\beta ~t$ $\alpha_z(t) = (-2)(0.800~rad/s^3)~t$ $\alpha_z(t) = (-1.60~rad/s^3)~t$ (b) When t = 3.00 s: $\alpha_z = (-1.60~rad/s^3)(3.00~s)$ $\alpha_z = -4.80~rad/s^2$ When t = 0: $\omega_z(t) = \gamma -\beta ~t^2$ $\omega_z(t) = (5.00~rad/s) -(0.800~rad/s^3)(0)^2$ $\omega_z(t) = 5.00~rad/s$ When t = 3.00 s: $\omega_z(t) = \gamma -\beta ~t^2$ $\omega_z(t) = (5.00~rad/s) -(0.800~rad/s^3)(3.00~s)^2$ $\omega_z(t) = -2.20~rad/s$ We can find the average angular acceleration. $\alpha_{ave} = \frac{\omega_2-\omega_1}{t}$ $\alpha_{ave} = \frac{(-2.20~rad/s)-(5.00~rad/s)}{3.00~s}$ $\alpha_{ave} = -2.40~rad/s^2$ The instantaneous angular acceleration at t = 3.00 seconds is double the magnitude of the average angular acceleration between 0 and 3.00 seconds. The two quantities are different because the angular acceleration changes as a function of time. The angular acceleration is not constant.
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