Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 43 - Energy from the Nucleus - Problems - Page 1331: 13a

Answer

251 MeV

Work Step by Step

The electric potential energy associated with the two circular nuclei touching each other is given by $$ U=\frac{1}{4 \pi \varepsilon_{0}} \frac{Z_{\mathrm{Xe}} Z_{\mathrm{Sr}} e^{2}}{r_{\mathrm{Xe}}+r_{\mathrm{Sr}}} $$ where $Z_{\mathrm{Xe}}$ is the atomic number of xenon, $Z_{\mathrm{Sr}}$ is the atomic number of strontium, $r_{\mathrm{Xe}}$ is the radius of a xenon nucleus, and $r_{\mathrm{Sr}}$ is the radius of a strontium nucleus. The radii are given by $r=$ $(1.2 \mathrm{fm}) A^{1 / 3},$ where $A$ is the mass number. Where fm is fermi meter which is $10^{-15}$m The mass number of Xe = 140 and for Sr is 96 Using the above information, the following calculations can be done to calculate radius of Xe and Sr Thus, $$ r_{\mathrm{Xe}}=(1.2 \mathrm{fm})(140)^{1 / 3}=6.23 \mathrm{fm}=6.23 \times 10^{-15} \mathrm{m} $$ and $$ r_{\mathrm{Sr}}=(1.2 \mathrm{fm})(96)^{1 / 3}=5.49 \mathrm{fm}=5.49 \times 10^{-15} \mathrm{m} $$ Hence, the potential energy is $$ \begin{aligned} U &=\left(8.99 \times 10^{9} \mathrm{V} \cdot \mathrm{m} / \mathrm{C}\right) \frac{(54)(38)\left(1.60 \times 10^{-19} \mathrm{C}\right)^{2}}{6.23 \times 10^{-15} \mathrm{m}+5.49 \times 10^{-15} \mathrm{m}}=4.08 \times 10^{-11} \mathrm{J} \\ &=251 \mathrm{MeV} \end{aligned} $$
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