Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 6 - Work and Energy - General Problems - Page 167: 75

Answer

(a) $v = \sqrt{\frac{F\cdot x}{m}}$ (b)$v = \sqrt{\frac{3~F\cdot x}{4~m}}$

Work Step by Step

The force $F$ is equal to $kx$. The total energy $E$ in the system is $\frac{1}{2}kx^2$. These two equations can be written as: $k = \frac{F}{x}$ $E = \frac{1}{2}kx^2 = \frac{1}{2}F\cdot x$ (a) When $x=0$, all the of the energy in the system is in the form of kinetic energy. Therefore, $KE = E$ $\frac{1}{2}mv^2 = \frac{1}{2}F\cdot x$ $v^2 = \frac{F\cdot x}{m}$ $v = \sqrt{\frac{F\cdot x}{m}}$ (b) When the spring is stretched $\frac{x}{2}$, then 25% of the energy $E$ is elastic potential energy stored in the spring and 75% of the energy $E$ is kinetic energy. So, $KE = 0.75~E$ $\frac{1}{2}mv^2 = \frac{3}{4}\times \frac{1}{2}F\cdot x$ $v^2 = \frac{3~F\cdot x}{4~m}$ $v = \sqrt{\frac{3~F\cdot x}{4~m}}$
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