Published by Patrick Mutisya · 8 days ago
A β‑particle is a high‑speed electron that is emitted from the nucleus of an unstable atom. It is produced when a neutron in the nucleus is transformed into a proton and an electron (plus an antineutrino). The electron escapes the nucleus and is observed as the β‑particle.
The basic nuclear reaction for β‑decay can be written as:
\$n \;\rightarrow\; p^{+} + e^{-} + \bar{\nu}_{e}\$
where:
Because a neutron (no charge) becomes a proton (positive charge) and an electron leaves the nucleus, the atomic number \$Z\$ of the element increases by one while the mass number \$A\$ remains unchanged.
The general nuclear equation for β‑emission is:
\$^{A}{Z}\!X \;\rightarrow\; ^{A}{Z+1}\!Y \;+\; e^{-} \;+\; \bar{\nu}_{e}\$
where \$^{A}{Z}\!X\$ is the parent nuclide and \$^{A}{Z+1}\!Y\$ is the daughter nuclide.
| Feature | α‑Decay | β‑Decay |
|---|---|---|
| Particle emitted | Helium nucleus (\$^{4}_{2}\!He\$) | Electron (\$e^{-}\$) + antineutrino |
| Change in atomic number \$Z\$ | \$Z-2\$ | \$Z+1\$ |
| Change in mass number \$A\$ | \$A-4\$ | \$A\$ (unchanged) |
| Penetrating power (low → high) | Low | Medium |
| Typical speed of emitted particle | ~\$1.5\times10^{7}\,\text{m s}^{-1}\$ | ~\$2.0\times10^{8}\,\text{m s}^{-1}\$ (close to \$c\$) |
Carbon‑14 (\$^{14}_{6}\!C\$) undergoes β‑decay to become nitrogen‑14:
\$^{14}{6}\!C \;\rightarrow\; ^{14}{7}\!N \;+\; e^{-} \;+\; \bar{\nu}_{e}\$
Notice that the mass number stays at 14, while the atomic number increases from 6 (carbon) to 7 (nitrogen).
β‑decay is a process that reduces the number of excess neutrons in an unstable nucleus. A neutron transforms into a proton, emitting a high‑speed electron (β‑particle) and an antineutrino. The atomic number increases by one, the mass number stays constant, and the element changes to the next higher \$Z\$ in the periodic table.