Essential University Physics: Volume 1 (4th Edition)

Published by Pearson
ISBN 10: 0-134-98855-8
ISBN 13: 978-0-13498-855-9

Chapter 9 - Exercises and Problems - Page 172: 69

Answer

The proof is below.

Work Step by Step

We first find the velocity that would cause the cars to slide this far: $\frac{1}{2}mv^2 = F_f \times \Delta x$ $\frac{1}{2}mv^2 = mg \mu \Delta x$ $v=\sqrt{2g \mu \Delta x}=13.1\ m/s=47.19 \ km/h$ This means that the initial momentum must have been: $=(2140+1040)(47.19)=150,062$ The slowest possible speed scenario would be if the large car possessed most of this momentum. Thus, we find: $150062 =\sqrt{(2140^2v^2+1040^2(55^2)}$ $v=64.82 \ km/h$ Thus, it is clear that at least one of the cars was speeding.
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.