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 8 - Dynamics II: Motion in a Plane - Conceptual Questions - Page 210: 9

Answer

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Work Step by Step

To understand this situation, we need to draw the force diagram exerted on the ball while it is moving in a vertical circle. At the top of the circle, the two forces exerted on the ball are both downward, its own weight, and the tension in the string. $$\sum F_y=F_G+T=ma_r=\dfrac{mv^2}{R}$$ $$F_G+T=\dfrac{mv^2}{R}$$ where $R$ is the radius of the circle which is the length of the string, $m$ is the ball's mass, and $v$ is its speed. Thus, at a minimum speed, $T=0\;\rm N$ if we are rotating at a minimum speed that just allows it to complete the vertical loop, the tension force in the string attached to it is then zero. $$\overbrace{F_G}^{=mg} =\dfrac{mv^2}{R}\tag 1$$ Thus, the minimum velocity required for the ball to complete the vertical loop is given by $$ { \color{red}{\bf\not}mg} =\dfrac{\color{red}{\bf\not}mv^2}{R}$$ $$v =\sqrt{Rg}$$ Any speed less than that, the ball will be under the free-fall acceleration with some horizontal velocity component which allowed it to move as a projectile that is fired from the top of the vertical circle.
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