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 1175: 22

Answer

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Work Step by Step

In this problem, the electron is initially moving in the $z $-direction with no velocity component in the $x $-direction ($v_x = 0 \;\rm{m/s} $). The question asks whether $v_x $ will still be zero after the electron passes through the hole in the barrier or not. This is a case involving the Heisenberg Uncertainty Principle, which relates the uncertainty in position $\Delta x $ and the uncertainty in momentum $\Delta p_x $ where $$ \Delta x \cdot \Delta p_x \geq \frac{h}{2}\tag 1 $$ The electron passes through a 10-$\mu$m-diameter circular hole. This means that the uncertainty in the electron's position in the $x $-direction ($\Delta x $) is approximately the diameter of the hole: $$ \Delta x \approx 10 \;\mu\rm{m} = \bf 10 \times 10^{-6} \;\rm{m}\tag2 $$ Solving (1) for $\Delta p_x$ $$ \Delta p_x \geq \frac{h}{2 \Delta x}\tag 3 $$ The uncertainty in velocity $\Delta v_x $ can be found by $$ \Delta p_x = m_e \Delta v_x $$ Plug into (3); $$m_e \Delta v_x\geq \frac{h}{2 \Delta x} $$ Hence, $$ \Delta v_x \geq \frac{h}{2m_e \Delta x} $$ Plug the known; $$ \Delta v_x \geq \frac{(6.63\times 10^{-34})}{2(9.11\times 10^{-31}) (10 \times 10^{-6})}=\bf 36.4\;\rm m/s $$ Thus, $$ \Delta v_x \geq\bf 36\;\rm m/s $$ After the electron passes through the hole, it is not certain that $v_x $ is still zero. And since the the average velocity in the $x$-directionis zero, So $$\boxed{-18\;{\rm m/s}\leq 18\leq \;{\rm m/s}}$$
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