Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 39 - Wave Functions and Uncertainty - Exercises and Problems - Page 1176: 28

Answer

a) $\rm 8 \;cycles$ b) From ${\bf 0.938\;\rm MHz} $ to ${\bf 1.03\;\rm MHz}$

Work Step by Step

$$\color{blue}{\bf [a]}$$ The number of complete cycles in one pulse is given by $$N={\rm\dfrac{Pulse\;length}{Wave\;length}}=\dfrac{L}{\lambda}$$ where $\lambda=v/f$; $$N =\dfrac{Lf}{v}$$ Plug the known; $$N =\dfrac{(12\times 10^{-3})(1\times 10^6)}{(1500)}=\color{red}{\bf 8}\;\rm cycles$$ $$\color{blue}{\bf [b]}$$ To find the range of frequencies, or bandwidth, needed to create this pulse, we need to use the concept of the uncertainty principle for signals. $$\Delta f \approx \frac{1}{\Delta t}\tag 1$$ The pulse duration, in our case, is given by $$ \Delta t = 8 T_{\lambda} =\dfrac{8}{f}$$ Plug the known; $$\Delta t=\dfrac{8}{(1\times 10^6)}=\bf 8\times 10^{-6}\;\rm s$$ Plug into (1), $$\Delta f \approx \frac{1}{ 8\times 10^{-6}}=\bf 1.25\times 10^{5}\;\rm Hz\tag 2$$ Hence the range of frequencies that is needed to be superimposed to create this pulse is given by $$ \left[f-\frac{1}{2}\Delta f \right] \leq f\leq\left[ f+\frac{1}{2}\Delta f \right]$$ Plug the known from (2) and from the given; $$ \left[(1.0\times 10^{6})-\frac{1}{2}(1.25\times 10^{5}) \right] \leq f\leq \left[(1.0\times 10^{6})+\frac{1}{2}(1.25\times 10^{5}) \right]$$ $$ {\bf 0.938\;\rm MHz} \leq f\leq{\bf 1.03\;\rm MHz}$$
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