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 297: 9.54

Answer

$I = \frac{1}{3}ML^2$

Work Step by Step

Equation (9.20) states: $I = \int~r^2~dm$. Let $\rho$ be the length density of the disk. $I = \int_{0}^{L}~r^2~\rho~(dr)$ $I = \rho\int_{0}^{L}~r^2~dr$ $I = \rho~(\frac{r^3}{3})\vert_{0}^{L}$ $I = \rho~(\frac{L^3}{3})$ $I = \frac{1}{3}~\rho~(L)~L^2$ $I = \frac{1}{3}ML^2$
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