University Calculus: Early Transcendentals (3rd Edition)

Published by Pearson
ISBN 10: 0321999584
ISBN 13: 978-0-32199-958-0

Chapter 12 - Section 12.6 - Velocity and Acceleration in Polar Coordinates - Exercises - Page 672: 3

Answer

$v=2a e^{a \theta}u_r+2e^{a \theta}u_{\theta}$ and $a=4e^{a \theta}(a^2 -1)u_r+8a e^{a \theta} u_{\theta}$

Work Step by Step

The velocity in terms of $u_r$ and $u_{\theta}$ can be found as: $v=r_t u_r+r \theta_t u_{\theta}$ The acceleration in terms of $u_r$ and $u_{\theta}$ can be found as: $a=(\dfrac{d^2r}{dt^2}-r\theta^{.2})u_r+(r\theta^{..} +2r^{.}\theta^{.})u_{\theta}$ $\dfrac{d \theta}{dt}=\theta^{.}=2$ and $\theta^{..}=0$ So, $v=2a e^{a \theta}u_r+2e^{a \theta}u_{\theta}$ $a=(\dfrac{d^2r}{dt^2}-r\theta^{.2})u_r+(r\theta^{..} +2r^{.}\theta^{.})u_{\theta}=4e^{a \theta}(a^2 -1)u_r+8a e^{a \theta} u_{\theta}$
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.