When protons and neutrons (nucleons) stick together to form a nucleus, the total mass of the nucleus is a little *less* than the sum of the masses of the individual nucleons. That missing mass is called the mass defect (Δm). It is converted into binding energy that holds the nucleus together.
Think of nucleons as Lego bricks. When you snap them together, a little bit of the bricks’ mass “disappears” because the bricks are now glued together more tightly – that’s the mass defect.
The binding energy per nucleon is the average energy that keeps each nucleon in the nucleus. It is calculated as:
\$\text{BE per nucleon} = \frac{\Delta m \, c^2}{A}\$
Where A is the mass number (total nucleons). A higher value means a more tightly bound nucleus.
| Isotope | Binding Energy (MeV) | BE per Nucleon (MeV) |
|---|---|---|
| \$^1\$H | 0 | 0 |
| \$^4\$He | 28.3 | 7.1 |
| \$^{12}\$C | 92.2 | 7.7 |
| \$^{56}\$Fe | 492.2 | 8.8 |
| \$^{238}\$U | 1780 | 7.5 |
Fusion (e.g., \$^1\$H + \$^1\$H → \$^4\$He) moves from low BE per nucleon (0) to higher (≈7 MeV). The difference is released as energy. This is how the Sun shines. 🌞
Fission (e.g., \$^{235}\$U → \$^{140}\$Xe + \$^{94}\$Kr) splits a heavy nucleus into two lighter ones with higher BE per nucleon (≈7.5 MeV). The energy difference powers nuclear reactors. ⚡
Both processes involve moving toward the peak of the binding‑energy curve (around iron). The closer you get to the peak, the more energy you can release.