University Physics with Modern Physics (14th Edition)

Published by Pearson
ISBN 10: 0321973615
ISBN 13: 978-0-32197-361-0

Chapter 43 - Nuclear Physics - Problems - Exercises - Page 1479: 43.71

Answer

$R = 4.59 \times 10^{-5} g/h$

Work Step by Step

$A = A_oe^{-\lambda t}$ and $\lambda = \frac{ln2}{T_{1/2}}$ * side note: $1 \space ci = 3.7 \times 10^{10} s^{-1} Ci^{-1}$ can be used later in conversion. The activity after 1000 hours is $A_{1000h} = A_oe^{-\frac{tln2}{T_{1/2}}}$ $A_{1000h} =(9.4 \times 10^{-6} Ci )( 3.7 \times 10^{10} s^{-1} Ci^{-1}) e^{-\frac{(1000h)ln2}{(45d)(24h/d)}}$ $A_{1000h} =1.8306 \times 10^5 Bq$ The activity is 84 Bq current activity = $\frac{A}{A_{1000h}}$ current activity =$ \frac{84 Bq}{1.8306 \times 10^5 Bq}$ current activity =$ 4.5886 \times 10^{-4} $ Now at 84 Bq, the mass fraction within the activity is $m_f = current \space activity \times m$ $m_f = 4.5886 \times 10^{-4} \times 100g$ $m_f = 4.59 \times 10^{-2} g$ This mass fraction is divided by 1000h because it is the total time elapsed in the test. The rate at which the piston rings lost their mass is $R = \frac{m_f}{1000h}$ $R = \frac{4.59 \times 10^{-2} g}{1000h}$ $R = 4.59 \times 10^{-5} g/h$
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