Physics Technology Update (4th Edition)

Published by Pearson
ISBN 10: 0-32190-308-0
ISBN 13: 978-0-32190-308-2

Chapter 32 - Nuclear Physics and Nuclear Radiation - Problems and Conceptual Exercises - Page 1153: 34

Answer

$1.3\mu Ci$

Work Step by Step

We know that $\lambda=\frac{\ln 2}{T_{\frac{1}{2}}}$ $\lambda=\frac{0.693}{6.05h}=0.115/h$ $Number\space of\space nuclei \space N=\frac{R}{\lambda}$ $N=\frac{1.5\times 10^{-6}Ci}{0.115/h}$ $N=(1.5\times 10^{-6}Ci)(\frac{1}{0.155/h})(\frac{3600s}{h})(\frac{3.7\times 10^{10}decay/s}{1Ci})=1.74\times 10^9nuclei$ Now the required activity can be determined as $R=\lambda N_{\circ}e^{-\lambda}t$ We plug in the known values to obtain: $R=(0.115/h)(1.744\times 10^9)e^{-\frac{0.115/h}{2.05h}}(\frac{1h}{3600s})(\frac{1ci}{3.7\times 10^{10}decay/s})$ $R=1.3\mu Ci$
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