University Physics with Modern Physics (14th Edition)

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

Chapter 5 - Applying Newton's Laws - Problems - Exercises - Page 162: 5.28

Answer

(a) $F_f = 0$ (b) $F_f = 6.0~N$ (c) $F = 16.0~N$ (d) $F = 8.0~N$ (e) $F_f = 8.0~N$ $a = 2.45~m/s^2$

Work Step by Step

(a) If the box is at rest and no horizontal force is applied to the box, then the friction force is zero. (b) If a horizontal force of 6.0 N is applied to the box, the force of static friction, which opposes this force, is 6.0 N. (c) We can find the maximum possible force of static friction. $F_f = F_N ~\mu_s = (40.0~N)(0.40)$ $F_f = 16.0~N$ The maximum possible force of static friction is 16.0 N. If the horizontal force is greater than 16.0 N then the box will start moving. (d) The minimum force $F$ to keep the box moving will be equal in magnitude to the force of kinetic friction. $F = F_N~\mu_k = (40.0~N)(0.20) = 8.0~N$ (e) We can find the mass of the box. $40.0 ~N = mg$ $m = \frac{40.0~N}{9.80~m/s^2} = 4.08~kg$ As we found in part (d), the magnitude of the force of kinetic friction is 8.0 N. We can find the acceleration of the box. $\sum F = ma$ $F-F_f = ma$ $a = \frac{18.0~N - 8.0~N}{4.08~kg}$ $a = 2.45~m/s^2$
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.