State that during α‑decay or β‑decay** the atomic number \$Z\$ of the nucleus changes, so the daughter nucleus is a different chemical element.
An element is defined solely by its atomic number \$Z\$ (the number of protons). Any change in \$Z\$ therefore means a change of element, irrespective of the mass number \$A\$.
“Radioactive decay is a change in an unstable nucleus that can result in the emission of α‑particles or β‑particles and/or γ‑radiation; the change is spontaneous and random**.”
Both statements are now explicitly included in the notes.
\$n \;\rightarrow\; p + ^{0}{-1}\beta + \bar{\nu}{e}\$
\$p \;\rightarrow\; n + ^{0}{+1}\beta^{+} + \nu{e}\$
\$p + e^{-} \;\rightarrow\; n + \nu_{e}\$
Both processes reduce \$Z\$ by 1.
| Decay | Change in \$Z\$ | Change in \$A\$ | Daughter Nucleus |
|---|---|---|---|
| α‑decay | –2 (two protons leave) | –4 (two protons + two neutrons leave) | \$^{A-4}_{Z-2}\text{Y}\$ |
| β⁻‑decay | +1 (neutron → proton) | 0 (mass unchanged) | \$^{A}_{Z+1}\text{Y}\$ |
| β⁺‑decay / Electron capture | –1 (proton → neutron) | 0 (mass unchanged) | \$^{A}_{Z-1}\text{Y}\$ |
| Parent Nuclide | Decay Type | Nuclear Equation | Daughter Element |
|---|---|---|---|
| \$^{238}_{92}\text{U}\$ | α | \$^{238}{92}\text{U} \;\rightarrow\; ^{234}{90}\text{Th} + ^{4}_{2}\text{He}\$ | U → Th (Z: 92 → 90) |
| \$^{14}_{6}\text{C}\$ | β⁻ | \$^{14}{6}\text{C} \;\rightarrow\; ^{14}{7}\text{N} + ^{0}{-1}\beta + \bar{\nu}{e}\$ | C → N (Z: 6 → 7) |
| \$^{22}_{11}\text{Na}\$ | β⁺ (supplementary) | \$^{22}{11}\text{Na} \;\rightarrow\; ^{22}{10}\text{Ne} + ^{0}{+1}\beta^{+} + \nu{e}\$ | Na → Ne (Z: 11 → 10) |
| \$^{40}_{19}\text{K}\$ | β⁻ (primary, with a rare α branch) | \$^{40}{19}\text{K} \;\rightarrow\; ^{40}{20}\text{Ca} + ^{0}{-1}\beta + \bar{\nu}{e}\$ | K → Ca (Z: 19 → 20) |
For calculations involving half‑life, decay constant and activity, see Section 5.2.4 – Radioactive Decay Calculations.
When working with radioactive sources, always apply the three protective principles: time (minimise exposure), distance (stay as far as practical), and shielding** (use appropriate material such as lead or concrete).
Both α‑decay and β‑decay alter the atomic number \$Z\$ of the nucleus (by –2, +1, or –1). Because \$Z\$ uniquely defines an element, the daughter nucleus is always a different element from the parent. The accompanying change (or lack of change) in mass number \$A\$ follows the patterns shown above, enabling students to construct correct nuclear equations, locate the daughter nuclide on the periodic table, and recognise that all decays are spontaneous and random, as required by the Cambridge IGCSE syllabus.
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