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: 46

Answer

(a) $12.13~MeV$ (b) $15.66~MeV$ (c) Neutron

Work Step by Step

(a) We know that $\Delta m=16.007934u-15.994915u=0.013019u$ Now the required energy can be determined as $E=|\Delta m|c^2$ We plug in the known values to obtain: $E=(0.013019u)|\frac{931.494\frac{MeV}{c^2}}{1u}|c^2$ $\implies E=(0.013019)(931.494MeV)=12.13MeV$ (b) We know that $\Delta m=m_f-m_i$ $\Delta m=16.01173u-15.994915u=0.016815u$ Now, $E=|\Delta m|c^2$ $\implies E=(0.016815u)|\frac{931.494\frac{MeV}{c^2}}{1u}|c^2$ $\implies E=15.66MeV$ (c) We can see from the results of part(a) and part(b) that the energy required to remove a neutron from a nucleus is greater than that of proton. The reason behind this is that the neutron is more strongly bound to the nucleus than a proton. Thus, we conclude that neutron removal needs more energy.
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