Physics Technology Update (4th Edition)

Published by Pearson
ISBN 10: 0-32190-308-0
ISBN 13: 978-0-32190-308-2

Chapter 17 - Phases and Phase Changes - Problems and Conceptual Exercises - Page 608: 86

Answer

(a) $1.6\times 10^{-4}m$ (b) $2.9\times 10^{-4}m$

Work Step by Step

(a) We know that at the top of the circle, the tension in the wire is given as $F=m(\frac{v^2}{r}-g)$ $\implies F=1.078Kg(\frac{(7.8m/s)^2}{0.852m}-9.8m/s^2)$ $\implies F=66.4Kg.m^2/s^2$ Now the stretch in the wire can be determined as $\Delta L=\frac{FL_{\circ}}{YA}$ We plug in the known values to obtain: $\Delta L=\frac{(66.4N)(0.82m)}{(6.9\times 10^{10}N/m^2)(\frac{\pi}{4}d^2)}$ $\implies \Delta L=1.6\times 10^{-4}m$ (b) We know that the tension at the bottom of the circle is given as $F^{\prime}=m(\frac{v^2}{r}+g)$ We plug in the known values to obtain: $F^{\prime}=(1.078Kg)(\frac{(9.3m/s)^2}{0.852m}+9.8m/s^2)$ $F^{\prime}=120N$ Now $\Delta L^{\prime}=\frac{F^{\prime}L_{\circ}}{YA}$ We plug in the known values to obtain: $\Delta L^{\prime}=\frac{(120N)(0.82m)}{(6.9\times 10^{10}N/m^2)(4.9\times 10^{-6}m^2)}=2.9\times 10^{-4}m$
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