i. Binding energy per nucleon (\(\bar B\)), for nucleus containing (A) nucleons with binding energy (B.E.) is given as,
\(\bar B\) = B.E./A
ii. Mean binding energy per nucleon (\(\bar B\)) for the most stable isotopes as a function of mass number is shown above. This plot leads to the following inferences :
a. Light nuclides :
(A < 30)
The peaks with A values in multiples of 4.
For example,
\(_2^4He\), \(_6^{12}C\),\(_8^{16}O\) are more stable.
b. Medium mass nuclides :
(30 < A < 90)
\(\bar B\) increases typically from 8 MeV for A = 16 to nearly 8.3 MeV for A between 28 and 32 and it remains nearly constant 8.5 MeV beyond this and shows a broad maximum. The nuclides falling on the maximum are most stable which turns possess high values. 56Fe with \(\bar B\) value of 8.79 MeV is the most stable.
c. Heavy nuclides :
(A > 90)
\(\bar B\) decreases from maximum 8.79 MeV to 7.7 MeV for A ≅ 210, 209Bi is the stable nuclide. Beyond this, all nuclides are radioactive (αemitters).