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 42 - Nuclear Physics - Exercises and Problems - Page 1276: 56

Answer

${\bf 3.6}\;\rm day$

Work Step by Step

To determine the effective half-life of the isotope in a patient's body, we need to consider both the radioactive decay and the excretion processes, which work together to remove the isotope. This is similar to calculating the combined effect of two processes running in parallel. The rate of removal from the body, $ \frac{dN}{dt} $, is the sum of the decay rate and the excretion rate: $$ \frac{dN}{dt} = \left( \frac{dN}{dt} \right)_{\text{decay}} + \left( \frac{dN}{dt} \right)_{\text{excrete}} $$ So, $$ \frac{dN}{dt} = -r_d N - r_e N = -(r_d + r_e) N $$ - Here, $ r_d $ is the decay rate, and $ r_e $ is the excretion rate. The effective removal rate $ r_{\text{eff}} $ is the sum of $ r_d $ and $ r_e $, $$ r_{\text{eff}} = r_d + r_e \tag 1$$ $$ \frac{dN}{dt} = -r_{\text{eff}} N $$ Recalling that $$ r = \frac{\ln(2)}{t_{1/2}} $$ Thus, the effective decay constant $ r_{\text{eff}} $ can be written as: $$ r_{\text{eff}} = \frac{\ln(2)}{(t_{1/2})_\text{decay}} + \frac{\ln(2)}{(t_{1/2})_\text{excrete}} $$ Recalling that $r=\ln(2)/t_{1/2}$, so from (1) $$ \frac{\color{red}{\bf\not} \ln(2)}{(t_{1/2})_\text{eff}} = \frac{\color{red}{\bf\not} \ln(2)}{ (t_{1/2})_\text{decay}} + \frac{\color{red}{\bf\not} \ln(2)}{(t_{1/2})_\text{excrete}} $$ $$ \frac{1}{(t_{1/2})_\text{eff}} = \frac{ 1}{ (t_{1/2})_\text{decay}} + \frac{1}{(t_{1/2})_\text{excrete}} $$ Substitute the given values of $(t_{1/2})_\text{decay} = 9.0 $ days and $(t_{1/2})_\text{excrete}= 6.0 $ days) $$ (t_{1/2})_\text{eff} = \left[\frac{1}{9.0 } + \frac{1}{6.0 }\right]^{-1} $$ $$ (t_{1/2})_\text{eff} = \color{red}{\bf 3.6}\;\rm day $$
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