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: 92

Answer

x = 240 m

Work Step by Step

We can use a force equation to find the acceleration while the skier is on the incline: $ma = \sum F$ $ma = mg ~sin(\theta) - mg ~cos(\theta)\cdot \mu_k$ $a = g ~sin(\theta) - g ~cos(\theta)\cdot \mu_k$ $a = (9.80 ~m/s^2) ~sin(28^{\circ}) - (9.80 ~m/s^2) ~cos(28^{\circ}) \cdot (0.18)$ $a = 3.04~m/s^2$ We can use kinematics to find the velocity $v$ at the bottom of the incline: $v^2 = v_0^2 + 2ax$ $v = \sqrt{v_0^2 + 2ax}$ $v = \sqrt{(5.0 ~m/s)^2 + (2)(3.04 ~m/s^2)(110 ~m)}$ $v = 26.3 ~m/s$ We can use a force equation to find the rate of deceleration while the skier is on the flat surface: $ma = \sum F$ $ma = mg ~ \mu_k$ $a = g ~ \mu_k$ $a = (9.80 ~m/s^2)(0.15)$ $a = 1.47~m/s^2$ We can use kinematics to find the distance $x$ that the skier travels along the flat surface. We can use $v_0 = 26.3 ~m/s$ for this part of the question: $x = \frac{v^2 - v_0^2}{2a} = \frac{0 - (26.3 ~m/s)^2}{(2)(-1.47 ~m/s^2)} = 240 ~m$
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.