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: 11

Answer

$ ^{16}\text{O} $ is more tightly bound.

Work Step by Step

To calculate and compare the binding energy per nucleon for $ ^{14}\text{O} $ and $ ^{16}\text{O} $, we’ll apply the formula for nuclear binding energy: $$ B =( Z m_H + N m_n - m_{\text{atom}})(931.49 \, \text{MeV/u})\tag 1 $$ where: - $ Z $ is the number of protons, - $ m_H $ is the mass of a proton, - $ N $ is the number of neutrons, - $ m_n $ is the mass of a neutron, - $ m_{\text{atom}} $ is the mass of the nucleus. The resulting binding energy $ B $ is then divided by the total number of nucleons to find the binding energy per nucleon. For $ ^{14}\text{O} $: $Z=8$, $N=8$, and $ m_{\text{atom}}=\rm 14.008595 \;u$ Plug into (1); $$ B_{ ^{14}\text{O} } =\left[ 8(1.007825 \, \text{u}) + 6(1.008665 \, \text{u}) - 14.008595 \, \text{u}\right](931.49 \, \text{MeV/u}) $$ $$ B_{ ^{14}\text{O} } =\color{blue}{\bf 98.7333}\, \text{MeV} $$ Binding energy per nucleon for $ ^{14}\text{O} $: $$ \dfrac{B_{ ^{14}\text{O} }}{{\rm nucleon }}=\frac{98.7333\, \text{MeV}}{14} =\color{red}{\bf 7.0524}\, \text{MeV} $$ --- For $ ^{16}\text{O} $: $Z=8$, $N=8$, and $ m_{\text{atom}}=\rm 15.994915\; u$ Plug into (1); $$ B_{^{16}\text{O} } =\left[ 8(1.007825 \, \text{u}) + 8(1.008665 \, \text{u}) - 15.994915\, \text{u}\right](931.49 \, \text{MeV/u}) $$ $$ B_{^{16}\text{O} } =\color{blue}{\bf 127.619}\, \text{MeV} $$ Binding energy per nucleon for $ ^{16}\text{O} $: $$ \dfrac{B_{ ^{16}\text{O} }}{{\rm nucleon }}\frac{127.619\, \text{MeV}}{16} = \color{red}{\bf 7.9762}\, \text{MeV} $$ The binding energy per nucleon for $ ^{16}\text{O} \approx 7.98 \;\rm MeV$ is higher than the $ ^{14}\text{O} \approx 7.05 \;\rm MeV$. Therefore, $ ^{16}\text{O} $ is more tightly bound.
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