Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 4 - Dynamics: Newton's Laws of Motion - General Problems - Page 107: 91

Answer

(a) $a = 0.88 ~m/s^2$ (b) $a = 0.98 ~m/s^2$ (c) The smaller force of friction results in a faster rate of acceleration.

Work Step by Step

(a) $ma = \sum F$ $ma = F_T - F_f$ $a = \frac{F_T-F_f}{m}$ $a = \frac{240 ~N - (72 ~kg)(9.80 ~m/s^2)\cdot 0.25}{72 ~kg} = 0.88 ~m/s^2$ (b) We can find the normal force $F_N$ which the water exerts on the skier. $F_N + F_T ~sin(\theta) = mg$ $F_N = (72 ~kg)(9.80 ~m/s^2) - 240 ~sin(12^{\circ})$ $F_N = 656 ~N$ We can use a force equation to find the acceleration. $ma = \sum F$ $ma = F_T ~cos(\theta) - F_f$ $a = \frac{F_T ~cos(\theta) - F_N \cdot \mu_k}{m}$ $a = \frac{240 ~N \cdot cos(12^{\circ}) - (656 ~N)\cdot 0.25}{72 ~kg} = 0.98 ~m/s^2$ (c) The vertical component of the tension reduces the normal force between the skier and the water. This results in a smaller force of friction. Although the horizontal component of the tension is also slightly reduced, the smaller friction force results in a faster rate of acceleration.
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