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 40 - One-Dimensional Quantum Mechanics - Exercises and Problems - Page 1214: 38

Answer

${\bf 1.02 }\; \text{fm}$

Work Step by Step

We know that the penetration distance is given by $$ \eta = \frac{\hbar}{\sqrt{2m(U_0 - E)}} $$ We also know that $ \hbar = 1.05 \times 10^{-34} \; \text{J} \cdot \text{s} $, and the mass of the neutron is $ m = 1.67 \times 10^{-27} \; \text{kg} $. Plug into the formula above. $$ \eta = \frac{1.05 \times 10^{-34}}{\sqrt{2(1.67 \times 10^{-27})(U_0 - E)}}\tag 1 $$ From Figure 40.17 we can say that: the neutron is trapped in a finite square potential well, and the well's potential depth is $ 50 \; \text{MeV} $, but our neutron is only $ 20 \; \text{MeV} $ below the top of the potential well. Thus, $$ U_0 - E = 0-(-20)=20 \; \text{MeV} \text{J} $$ Plug into (1); $$ \eta = \frac{1.05 \times 10^{-34}}{\sqrt{2(1.67 \times 10^{-27})(20\times 1.6\times 10^{-19} )}} =\bf 1.02 \times 10^{-12}\;\rm m$$ $$ \eta =\color{red}{\bf 1.02 }\; \text{fm} $$
Update this answer!

You can help us out by revising, improving and updating this answer.

Update this answer

After you claim an answer you’ll have 24 hours to send in a draft. An editor will review the submission and either publish your submission or provide feedback.