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: 4

Answer

$v=a \cos t u_r +a(1+\sin t) e^{-t} u_{\theta}$ and $a(t)=-a(\sin t +(1+\sin t) e^{-2t})u_r-ae^{-t} (1+\sin t -2 \cos t) u_{\theta}$

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: $a=(\dfrac{d^2r}{dt^2}-r\theta^{.2})u_r+(r\theta^{..} +2r^{.}\theta^{.})u_{\theta}$ $\dfrac{d \theta}{dt}=\theta^{.}=e^{-t}$ and $\theta^{..}=-e^{-t}$ $\implies v (t)=a \cos t u_r +a(1+\sin t) e^{-t} u_{\theta}$ and $a(t)=(\dfrac{d^2r}{dt^2}-r\theta^{.2})u_r+(r\theta^{..} +2r^{.}\theta^{.})u_{\theta} \\ =-a(\sin t +(1+\sin t) e^{-2t})u_r-ae^{-t} (1+\sin t -2 \cos t) u_{\theta}$
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