University Physics with Modern Physics (14th Edition)

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

Chapter 7 - Potential Energy and Energy Conservation - Problems - Exercises - Page 235: 7.78

Answer

(a) (i) h = 0.925 m (ii) h = 1.06 m (iii) h = 2.43 m (b) h = 1.06 m (c) If $\theta$ increases, the speed at the bottom would increase.

Work Step by Step

(a) (i) $U+W = K$ $mgh - mg~cos(\theta)~\mu_k~\frac{h}{sin(\theta)} = \frac{1}{2}mv^2$ $gh - g~cot(\theta)~\mu_k~h = \frac{1}{2}v^2$ $h = \frac{v^2}{2~(g-g~cot(\theta)~\mu_k)}$ $h = \frac{(4.00~m/s)^2}{2~[9.80~m/s^2-9.80~m/s^2~cot(52.0^{\circ})(0.15)]}$ $h = 0.925~m$ (ii) $U+W = K$ $mgh - mg~cos(\theta)~\mu_k~\frac{h}{sin(\theta)} = \frac{1}{2}mv^2$ $gh - g~cot(\theta)~\mu_k~h = \frac{1}{2}v^2$ $h = \frac{v^2}{2~(g-g~cot(\theta)~\mu_k)}$ $h = \frac{(4.00~m/s)^2}{2~[9.80~m/s^2-9.80~m/s^2~cot(52.0^{\circ})(0.29)]}$ $h = 1.06~m$ (iii) (i) $U+W = K$ $mgh - mg~cos(\theta)~\mu_k~\frac{h}{sin(\theta)} = \frac{1}{2}mv^2$ $gh - g~cot(\theta)~\mu_k~h = \frac{1}{2}v^2$ $h = \frac{v^2}{2~(g-g~cot(\theta)~\mu_k)}$ $h = \frac{(4.00~m/s)^2}{2~[9.80~m/s^2-9.80~m/s^2~cot(52.0^{\circ})(0.85)]}$ $h = 2.43~m$ (b) Since the required height $h$ does not depend on the mass, the required height $h$ is still 1.06 meters. (c) If $\theta$ increases, the magnitude of the work done by friction decreases, so less energy is removed from the system. Therefore, the speed at the bottom would increase.
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.