Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 2 - Kinematics in One Dimension - Exercises and Problems - Page 67: 64

Answer

a) $24.5\;\rm m/s,\;34.6\;m/s$ b) $ a_x= \sqrt{\dfrac{ P }{2mt} } $ c) $3.87\;\rm m/s^2,\;1.22\;m/s^2$ d) It gives unreasonable values.

Work Step by Step

a) Since the car accelerates at the maximum possible rate during the first 20 s is modeled by $$v_x^2=\dfrac{2Pt}{m}$$ Thus, the speed of the car from 0 s to 20 s is given by $$v_x =\sqrt{\dfrac{2\cdot 3.6\times10^4 t}{1200}}$$ $$v_x=\sqrt{60t}\tag 1$$ Thus, at $t=10\;\rm s$, the speed is $$v_x =\sqrt{60\cdot 10}=\color {red}{\bf24.5}\;\rm m/s$$ And at $t=20\;\rm s$, the speed is $$v_x =\sqrt{60\cdot 20}=\color {red}{\bf 34.6}\;\rm m/s$$ b) To find the acceleration of the car in terms of $P$, $m$, and $t$, we need to differentiate the original formula relative to $t$. To make the derivative easy, we need to take $t$ out the square root since all other variables are constants. $$v_x =\sqrt{\dfrac{2P}{m}}\cdot t^{\frac{1}{2}}$$ $$\dfrac{d}{dt}v_x =\dfrac{d}{dt}\left(\sqrt{\dfrac{2P }{m} }\cdot t^{\frac{1}{2}}\right) $$ $$a_x=\left(\sqrt{\dfrac{2P }{m}}\right) \dfrac{d}{dt} \cdot t^{\frac{1}{2}}=\sqrt{\dfrac{2P }{m}}\cdot \frac{1}{2}t^{\frac{-1}{2}}$$ Thus, $$\boxed{a_x= \sqrt{\dfrac{ P }{2mt} } } $$ c) The acceleration at $t=1\;\rm s$; $$a_x= \sqrt{\dfrac{ P }{2mt} } = \sqrt{\dfrac{ 3.6\times10^4}{2\cdot 1200\cdot 1} }=\color{red}{\bf 3.87}\;\rm m/s^2$$ The acceleration at $t=10\;\rm s$; $$a_x= \sqrt{\dfrac{ P }{2mt} } = \sqrt{\dfrac{ 3.6\times10^4}{2\cdot 1200\cdot 10} }=\color{red}{\bf 1.22}\;\rm m/s^2$$ d) It fails because the smaller the $t$, the huge the acceleration. Let's take at $t=0.01\;\rm s$ to see the magnitude of the acceleration. $$a_x= \sqrt{\dfrac{ P }{2mt} } = \sqrt{\dfrac{ 3.6\times10^4}{2\cdot 1200\cdot 0.01} }=\color{blue}{\bf 38.7}\;\rm m/s^2$$ which is unreasonable value.
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