Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 8 - Potential Energy and Conservation of Energy - Problems - Page 210: 88b

Answer

-6.75 J

Work Step by Step

$F=mg=1.50\,kg\times9.8\,m/s^{2}=14.7\,N$ d= maximum height of the projectile=$\frac{(v_{0}\sin\theta_{0})^{2}}{2g}$ $=\frac{(3.00\,m/s\times\sin 90^{\circ})^{2}}{2\times9.8\,m/s^{2}}=0.459\,m$ Angle between force vector and displacement vector $\theta=180^{\circ}$ $W=Fd\cos\theta=14.7\,N\times0.459\,m\times\cos180^{\circ}=-6.75\,J$ The other method to solve this problem: $K_{1}=6.75\,J$ (from the previous section) $U_{1}=mgh_{1}=mg\times0=0$ $K_{2}=\frac{1}{2}mv_{f}^{2}=\frac{1}{2}m\times(0)^{2}=0$ $U_{2}=mgh_{2}$ According to the principle of conservation of mechanical energy, $K_{2}+U_{2}=K_{1}+U_{1}$ Therefore, we have $mgh_{2}=6.75\,J$ Now, $W=Fd\cos\theta=(mg)(h_{2})\cos180^{\circ}=-mgh_{2}=-6.75\,J$
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