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: 19

Answer

a) ${\bf 236} \, \rm{\mu g}$ b) ${\bf 140.3} \, \rm{\mu g}$ c) ${\bf 0.775} \, \rm{\mu g}$

Work Step by Step

We know that the radioactive decay is given by: $$ N = N_0 \left( \frac{1}{2} \right)^{t / t_{1/2}} $$ where: - $ N $ is the remaining quantity after time $ t $, - $ N_0 $ is the initial quantity ($250\;\rm \mu g $ in this case), - $ t $ is the elapsed time, - $ t_{1/2} $ is the half-life of the isotope (12 days for $^{131}\text{Ba}$, see appendix C). Now, we can find the remaining mass for each specified time period. $$\color{blue}{\bf [a]}$$ After $t=$1 Day: $$ N = 250 \left( \frac{1}{2} \right)^{1 / 12} \approx \color{red}{\bf 236} \, \rm{\mu g} $$ $$\color{blue}{\bf [b]}$$ After $t=$10 Day: $$ N = 250 \left( \frac{1}{2} \right)^{10 / 12} \approx \color{red}{\bf 140.3} \, \rm{\mu g} $$ $$\color{blue}{\bf [c]}$$ After $t=$100 Day: $$ N = 250 \left( \frac{1}{2} \right)^{100 / 12} \approx \color{red}{\bf 0.775} \, \rm{\mu g} $$
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