University Physics with Modern Physics (14th Edition)

Published by Pearson
ISBN 10: 0321973615
ISBN 13: 978-0-32197-361-0

Chapter 5 - Applying Newton's Laws - Problems - Exercises - Page 170: 5.115

Answer

$\frac{T_{B}}{T_{A}}$ =$ cos^{2}$$\beta$

Work Step by Step

Before the horizontal string is cut, the ball is in equilibrium, and the vertical component of the tension force must balance the weight, so $T_{A}$cos$\beta$ = W $T_{A}$=$\frac{W}{cos\beta}$ At point B, the ball is not in equilibrium; its speed is instantaneously 0, so there is no radial acceleration, and the tension force must balance the radial component of the weight so, $T_{B}$=$Wcos\beta$ Hence, $\frac{T_{B}}{T_{A}}$ =$ cos^{2}$$\beta$
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