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 1274: 20

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$$\color{blue}{\bf [a]}$$ Tritium ($ ^3 \rm{H} $) is a radioactive isotope of hydrogen, with an atomic number $ Z = 1 $ and a neutron count $ N = 2 $. This means that Tritium undergoes beta-minus ($ \beta^- $) decay, as seen in Appendix C. In this type of decay, a neutron in the nucleus transforms into a proton, emitting an electron (beta particle) and an antineutrino. Hence, tritium decays into the stable isotope of helium, $ ^3 \rm{He} $, through the reaction of $$ ^3 \rm{H} \to \;^3\rm{He} + \beta^- $$ Thus, the daughter nucleus of tritium decay is $\boxed{ ^3 \rm{He}} $. $$\color{blue}{\bf [b]}$$ The half-life ($ t_{1/2} $) of tritium is given as 12.33 years. Recalling that the decay rate, $ r $, can be calculated from the relationship: $$ r =\dfrac{1}{\tau}= \frac{\ln(2)}{t_{1/2}} $$ from $ N = N_0 \left( \frac{1}{2} \right)^{t / t_{1/2}} $; Substituting $ t_{1/2} = 12.33$ years, $$ r = \frac{\ln(2)}{12.33 \; \rm{years}} \times \frac{1 \; \rm{year}}{3.156 \times 10^7 \; \rm{s}} = \color{red}{\bf1.78 \times 10^{-9}} \; \rm{s}^{-1} $$ Therefore, the lifetime ($ \tau $) of tritium is given by $$ \tau = \frac{1}{r} = \frac{1}{1.83 \times 10^{-9} \; \rm{s}^{-1}} =\color{red}{\bf 5.614 \times 10^8 }\; \rm{s} $$
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