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 41 - Atomic Physics - Exercises and Problems - Page 1246: 47

Answer

a) $\ln(2)\;\tau$ b) ${\bf 11.8} \, \text{ns}$

Work Step by Step

$$\color{blue}{\bf [a]}$$ We know that the half-life $ t_{1/2} $ is the time required for half of the initially excited atoms to decay. $$ N_{\text{exc}}(t) = N_0 e^{-t/\tau}\tag 1 $$ This means that after the half-life $ t = t_{1/2} $, the number of excited atoms is half of the initial number: $$ N_{\text{exc}}(t_{1/2}) = \frac{1}{2} N_0 $$ Plug into (1); $$ \frac{1}{2} \color{red}{\bf\not}N_0= \color{red}{\bf\not}N_0 e^{-t/\tau}\tag 1 $$ Take the natural logarithm on both sides: $$ \ln\left(\frac{1}{2}\right) = -\frac{t_{1/2}}{\tau} $$ Since $ \ln\left(\frac{1}{2}\right) = -\ln(2) $, we have: $$ -\ln(2) = -\frac{t_{1/2}}{\tau} $$ Thus, the half-life is related to the lifetime $ \tau $ by: $$ \boxed{t_{1/2} = \tau \ln(2) } $$ $$\color{blue}{\bf [b]}$$ From Table 41.3, the lifetime $ \tau $ for the $ 3p $ state of sodium is $ \tau = 17 \, \text{ns} $. Plug that into the boxed formula above. $$ t_{1/2} = \ln(2) \times 17 \approx \color{red}{\bf 11.8} \, \text{ns} $$
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