Physics Technology Update (4th Edition)

Published by Pearson
ISBN 10: 0-32190-308-0
ISBN 13: 978-0-32190-308-2

Chapter 4 - Two-Dimensional Kinematics - Problems and Conceptual Exercises - Page 105: 25

Answer

$\textbf{(a)}$ $$\vec{g}=(-9.81\text{ m/s}^2)\hat{\bf y}.$$ $\textbf{(b)}$ $$v_0=1.13\text{ m/s}.$$ $\textbf{(c)}$ $$v_0'=3.21\text{ m/s}.$$

Work Step by Step

$\textbf{(a)}$ The acceleration is equal to the gravitational acceleration on the whole road, and thus just before the landing, as well. So it is of magnitude $g=9.81\text{ m/s}^2$ and pointing vertically downwards. $\textbf{(b)}$ Since the ball rolled off the table, its initial velocity is horizontal. The final vertical component of the velocity is thus: $$v_v=\sqrt{2gh}$$ The total landing speed is given by $$v^2=v_h^2+v_v^2=v_0^2+2gh,$$ where we used the fact that $v_h$ is equal to the initial speed. Now we get $$v_0^2=v^2-2gh$$ and finally $$v_0=\sqrt{v^2-2gh}=\sqrt{4.0^2-2\cdot9.81\cdot0.75}\text{ m/s}=1.13\text{ m/s}.$$ $\textbf{(c)}$ We will shorten our calculation by using the fact that no matter what is the initial ('horizontal') speed, if the height remains unchanged, the vertical component of the landing velocity will remain unchanged as well. So, we simply have, by analogy with the last formula $$v_0'=\sqrt{v'^2-2gh}=\sqrt{5.0^2-2\cdot9.81\cdot0.75}\text{ m/s}=3.21\text{ m/s}.$$
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.