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: 25

Answer

a) $\lambda_{2 \rightarrow 1} = \dfrac{8mL^2 c}{3h}$ b) $0.795\;\rm nm$

Work Step by Step

$$\color{blue}{\bf [a]}$$ In a rigid box (also called an infinite potential well), the energy levels of a particle are given by $$ E_n = \frac{n^2 h^2}{8mL^2} $$ So for a transition from $ n = 2 $ to $ n = 1 $ $$ \Delta E = E_2 - E_1 = \frac{4h^2}{8mL^2} - \frac{h^2}{8mL^2} = \frac{3h^2}{8mL^2} $$ Recalling that the energy of the emitted photon is equal to the energy difference, so $$ \Delta E=E_{\rm photon} $$ Thus, $$ \frac{3h^2}{8mL^2} = \frac{hc}{\lambda_{2 \rightarrow 1}} $$ Solve for $ \lambda_{2 \rightarrow 1} $: $$ \boxed{\lambda_{2 \rightarrow 1} = \frac{8mL^2 c}{3h}} $$ $$\color{blue}{\bf [b]}$$ To find the length of the box for a given wavelength of 694 nm, we need to solve the boxed formula above for $L$. So, $$ L^2 = \frac{3h \lambda_{2 \rightarrow 1}}{8mc} $$ $$ L = \sqrt{\frac{3h \lambda_{2 \rightarrow 1}}{8mc}} $$ Substitute the known; $$ L = \sqrt{\frac{3( 6.63 \times 10^{-34}) (694 \times 10^{-9} )}{8(9.11 \times 10^{-31})(3.0 \times 10^8)}}=\bf 7.95\times 10^{-10}\;\rm m $$ $$L=\color{red}{\bf 0.795}\;\rm nm$$
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.