Essential University Physics: Volume 1 (4th Edition)

Published by Pearson
ISBN 10: 0-134-98855-8
ISBN 13: 978-0-13498-855-9

Chapter 3 - Exercises and Problems - Page 53: 94

Answer

$\theta=cos^{-1}(\frac{\sqrt {Rg}}{V})$

Work Step by Step

Please see the attached image first. Let's apply equation $S=ut$ in the horizontal direction of AB motion. $\rightarrow S=ut+\frac{1}{2}at^{2}$ Let's plug known values into this equation. $2R=Vcos\theta\space t$ $\frac{2R}{Vcos\theta}= t-(1)$ Let's apply equation $S=ut+\frac{1}{2}at^{2}$ in vertical direction of AB motion. $\uparrow S=ut+\frac{1}{2}at^{2}$ Let's plug known values into this equation. $R=Vsin\theta\times t-\frac{1}{2}(-g)t^{2}-(2)$ $(1)=\gt(2),$ $-R=Vsin\theta\times \frac{2R}{Vcos\theta}-\frac{1}{2}(-g)(\frac{2R}{Vcos\theta})^{2} $ $-R= \frac{2Rsin\theta}{cos\theta}-\frac{2gR^{2}}{V^{2}cos^{2}\theta}-(3)$ The problem said that R is the horizontal range the projectile would have had if launched over level ground at the same launch angle. So we previously learned, $R=\frac{2V^{2}}{g}sin\theta cos\theta=\gt sin\theta=\frac{Rg}{V^{2}cos^{2}\theta}-(4)$ $(4)=\gt(3)$ $-R=(\frac{2R}{cos\theta})(\frac{Rg}{2V^{2}cos\theta})-(\frac{2R^{2}g}{V^{2}cos^{2}\theta})$ $-1=\frac{-Rg}{V^{2}cos^{2}\theta}$ $cos\theta = \sqrt {\frac{Rg}{V^{2}}}=\gt\theta=cos^{-1}(\frac{\sqrt {Rg}}{V})$
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