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 168: 5.95

Answer

The cart must have an acceleration of $\frac{g}{\mu_s}$ so the block does not fall. An observer on the cart would say that the block is at rest.

Work Step by Step

Let $m$ be the mass of the block. If the block does not fall, then the force of static friction directed up must be equal in magnitude to the weight of the block. $F_N~\mu_s = mg$ $F_N = \frac{mg}{\mu_s}$ We can use the normal force $F_N$ between the cart and the block to find the acceleration of the block. $\sum F = ma$ $F_N = ma$ $\frac{mg}{\mu_s} = ma$ $a = \frac{g}{\mu_s}$ The cart and the block must have the same acceleration. The cart must have an acceleration of $\frac{g}{\mu_s}$ so the block does not fall. An observer on the cart would say that the block is at rest.
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