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 6 - Dynamics I: Motion Along a Line - Exercises and Problems - Page 164: 61

Answer

a) $0\;\rm N$ b) $-222\;\rm N$

Work Step by Step

We know, from Newton's second law, that the net force is given by $$\sum F=ma$$ And since the only force exerted on the astronaut now is the spring force, $$F_{sp}=ma\tag 1$$ Now we need to find the acceleration of the astronaut by differentiating the given equation twice. We know that the position formula is given by $$x=0.3\sin(\pi t)$$ Thus, the speed is given by $$\dfrac{d}{dt}x=\dfrac{d}{dt}(0.3\sin(\pi t))$$ $$v =0.3\pi \cos(\pi t)$$ Hence, the acceleration is given by $$\dfrac{d}{dt}v=\dfrac{d}{dt}(0.3\pi \cos(\pi t))$$ $$a =-0.3\pi^2 \sin(\pi t)$$ Plugging into (1); $$F_{sp}=m \left[-0.3\pi^2 \sin(\pi t)\right]$$ $$F_{sp}= -0.3m\pi^2 \sin(\pi t) $$ a) At $t=1$ s: $$F_{sp}= -0.3\cdot 75\pi^2 \sin(\pi \cdot 1)=\color{red}{\bf 0}\;\rm N $$ a) At $t=1.5$ s: $$F_{sp}= -0.3\cdot 75\pi^2 \sin(\pi \cdot 1.5)=\color{red}{\bf -222}\;\rm N $$
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