Engineering Mechanics: Statics & Dynamics (14th Edition)

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

Chapter 17 - Planar Kinetics of a Rigid Body: Force and Acceleration - Section 17.1 - Mass Moment of Inertia - Problems - Page 419: 6

Answer

$\implies I_x=\frac{2}{5}mr^2$

Work Step by Step

We can determine the required moment of inertia as follows: We know that $dV=\pi y^2dx=\pi (r^2-x^2)dx$ $\implies dm=\rho dV$ $\implies dm=\rho \pi(r^2-x^2)dx$ $\implies m=\rho \pi \int_{-r}^r (r_2-x^2)dx$ $\implies m=\frac{4}{3}\pi \rho r^3$ [eq(1)] We also know that $dI=\frac{1}{2}y^2dm$ $\implies dI=\frac{1}{2}\rho \pi(r^2-x^2)^2dx$ $\implies I_x=\frac{1}{2}\pi \rho \int_{-r}^r (r^2-x^2)dx$ $\implies I_x=\frac{8}{15}\pi \rho r^5$ This can be rearranged as: $I_x=(\frac{4}{3}\pi \rho r^3)\frac{2}{5}r^2$ From eq(1) $m=\frac{4}{3}\pi \rho r^3$ $\implies I_x=\frac{2}{5}mr^2$
Update this answer!

You can help us out by revising, improving and updating this answer.

Update this answer

After you claim an answer you’ll have 24 hours to send in a draft. An editor will review the submission and either publish your submission or provide feedback.