Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 30 - Nuclear Physics and Radioactivity - Problems - Page 882: 36

Answer

$E_{release}=\left( M_{Parent}-M_{Daughter}-2m_e \right)c^2$.

Work Step by Step

The positron emission described is $^{A}_{Z}Parent \rightarrow\;^{A}_{Z-1}Daughter +\;^{0}_{1}e +\nu$. We add Z electrons to the left hand side, the parent nuclear mass, so that we may use the atomic mass. To balance the equation, we add Z electrons to the right hand side. We only need Z-1 electrons to be able to use the daughter’s atomic mass in our equation. We have 1 “extra” electron mass, and we also have the positron mass. In summary, on the right hand side, we have the daughter's atomic mass and 2 electron masses. Calculate the energy released. $$E_{release}=\left( M_{Parent}-(M_{Daughter}+2m_e) \right)c^2$$ $$E_{release}=\left( M_{Parent}-M_{Daughter}-2m_e \right)c^2$$ This was the relationship to be shown.
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