Physics (10th Edition)

Published by Wiley
ISBN 10: 1118486897
ISBN 13: 978-1-11848-689-4

Chapter 5 - Dynamics of Uniform Circular Motion - Problems - Page 141: 59

Answer

$\theta=28.1^o$

Work Step by Step

$\theta$ is the angle the string makes with the vertical. From this angle, the tension force $T$ in the string will have 2 components: horizontal one $T\sin\theta$ and vertical one $T\cos\theta$ After the block swings toward the outside of the curve, it makes an angle $\theta$ and stays put there. That means it does not have acceleration, and all net forces on the block equal $0$, meaning all forces balance one another. - Horizontal: $T\sin\theta$ opposes the centripetal force $F_c$, so $$T\sin\theta=F_c=\frac{mv^2}{r} (1)$$ - Vertical: $T\cos\theta$ opposes the block's weight $mg$, so $$T\cos\theta=mg (2)$$ From (1) and (2), we have $$\frac{T\sin\theta}{T\cos\theta}=\frac{\frac{mv^2}{r}}{mg}$$ $$\tan\theta=\frac{v^2}{rg}$$ We have $v=28m/s$, $r=150m$ and $g=9.8m/s^2$, so $$\tan\theta=0.533$$ $$\theta=28.1^o$$
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.