Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (4th Edition)

Published by Pearson
ISBN 10: 0133942651
ISBN 13: 978-0-13394-265-1

Chapter 10 - Interactions and Potential Energy - Exercises and Problems - Page 259: 57

Answer

(a) $x = \frac{\pi}{3}, \frac{2\pi}{3}$ (b) $x = \frac{\pi}{3}$ is an unstable equilibrium. $x = \frac{2\pi}{3}$ is a stable equilibrium.

Work Step by Step

(a) We can find the positions where $F = 0$: $F = -\frac{dU}{dx} = 0$ $-1-2~cos~2x = 0$ $cos~2x = -0.5$ $2x = cos^{-1}~(-0.5)$ $2x = \frac{2\pi}{3}, \frac{4\pi}{3}$ $x = \frac{\pi}{3}, \frac{2\pi}{3}$ (b) We can find an expression for $\frac{d^2U}{dx^2}$: $U(x) = x+sin~2x$ $\frac{dU}{dx} = 1+2~cos~2x$ $\frac{d^2U}{dx^2} = -4~sin~2x$ When $x = \frac{\pi}{3}$: $\frac{d^2U}{dx^2} = -4~sin~2x$ $\frac{d^2U}{dx^2} = -4~sin~[(2)(\frac{\pi}{3})]$ $\frac{d^2U}{dx^2} = -3.46$ When $x = \frac{\pi}{3},$ then $\frac{d^2U}{dx^2} \lt 0$, so this is a local maximum. $x = \frac{\pi}{3}$ is an unstable equilibrium. When $x = \frac{2\pi}{3}$: $\frac{d^2U}{dx^2} = -4~sin~2x$ $\frac{d^2U}{dx^2} = -4~sin~[(2)(\frac{2\pi}{3})]$ $\frac{d^2U}{dx^2} = 3.46$ When $x = \frac{2\pi}{3},$ then $\frac{d^2U}{dx^2} \gt 0$, so this is a local minimum. $x = \frac{2\pi}{3}$ is a stable equilibrium.
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