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Page Title: Binding Energy Per Nucleon (BE/A)
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Nuclear Physics and Reactor Theory Volume 1 of 2
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Summary

Atomic and Nuclear Physics DOE-HDBK-1019/1-93 NUCLEAR FISSION Binding  Energy  Per  Nucleon  (BE/A) As the number of particles in a nucleus increases, the total binding energy also increases.   The rate of increase, however, is not uniform.   This lack of uniformity results in a variation in the amount of binding energy associated with each nucleon within the nucleus.  This variation in the binding energy per nucleon (BE/A) is easily seen when the average BE/A is plotted versus atomic mass number (A), as shown in Figure 20. Figure 20    Binding Energy per Nucleon vs. Mass Number Figure 20 illustrates that as the atomic mass number increases, the binding energy per nucleon decreases for A > 60.   The BE/A curve reaches a maximum value of 8.79 MeV at A = 56 and decreases to about 7.6 MeV for A = 238.  The general shape of the BE/A curve can be explained using the general properties of nuclear forces.  The nucleus is held together by very short-range attractive forces that exist between nucleons.  On the other hand, the nucleus is being forced apart by long range repulsive electrostatic (coulomb) forces that exist between all the protons in the nucleus. Rev. 0 Page 53 NP-01

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