Physics (10th Edition)

Published by Wiley
ISBN 10: 1118486897
ISBN 13: 978-1-11848-689-4

Chapter 3 - Kinematics in Two Dimensions - Problems - Page 75: 43

Answer

$41.5^{\circ}$

Work Step by Step

By using trigonometry, we can get. $tan\theta=(\frac{2400\space m}{x})-(1)$ ; Where x is the horizontal displacement of the flare. Let's apply equation 3.5b $S=ut+\frac{1}{2}at^{2}$ in the vertical direction to find the flight time. $\uparrow S=ut+\frac{1}{2}at^{2}$ ; Let's plug known values into this equation. $-2400=-240sin30^{\circ}t+\frac{1}{2}(-9.8)t^{2}$ $4.9t^{2}+120t-2400=0$ ; This is a quadratic formula. So we can obtain the solutions as follows. $t=\frac{-120\space\pm\sqrt {(-120)^{2}-4(4.9)(-2400)}}{2(4.9)}=\frac{-120\space\pm247.9}{y}$ Here we neglect the negative solution & we get $t=13.05\space s$ Let's apply the equation $S=ut$ in the horizontal direction to find the x $\rightarrow S=ut$ ; Let's plug known values into this equation. $x=240\space m/s\times cos30^{\circ}\times13.05=2712.4\space m$ (1)=> $\theta=tan^{-1}(\frac{2400\space m}{2712.4\space m})=41.5^{\circ}$
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