Alpha, beta and gamma radiation (QCE Physics Unit 1)
“Describe the properties of alpha, beta and gamma radiation, including charge, mass, ionising and penetrating power, and represent decay reactions using balanced nuclear equations”
Alpha radiation is a He nucleus (charge , very strongly ionising, stopped by paper); beta-minus is a high-speed electron (charge , moderately ionising, stopped by aluminium); gamma is a high-energy photon (uncharged, weakly ionising, stopped by thick lead); and every decay equation must conserve both mass number and atomic number .
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What this dot point is asking
QCAA expects you to know the three classical types of ionising radiation (alpha, beta and gamma), the conservation laws governing decay equations, and the inverse relationship between ionising power and penetrating power.
The three types
| Type | Symbol | Composition | Charge | Mass (u) | Speed | Ionising power | Penetration | Shielding |
|---|---|---|---|---|---|---|---|---|
| Alpha | or | protons, neutrons | at most | Very strong | Very low | Sheet of paper, cm of air | ||
| Beta-minus | or | high-speed electron | up to | Moderate | Moderate | Few mm of aluminium | ||
| Gamma | high-energy photon | Weak | Very high | Thick lead or concrete |
Beta-plus (, the positron) also exists; it is the antiparticle of the electron and behaves with the same magnitudes but opposite charge.
Why ionising power and penetration are inverse
Alpha particles interact strongly because of their charge and slow speed; they deposit their energy quickly and stop in a short distance. Gamma photons have no charge and interact weakly; most pass through matter, so penetration is high but the dose deposited per metre is low.
Balanced nuclear equations
Two quantities are conserved in any nuclear decay or reaction:
- mass number (total number of nucleons),
- atomic number (total charge).
Alpha decay: drops by , drops by .
Beta-minus decay: A neutron becomes a proton plus an electron plus an antineutrino. unchanged, increases by .
Gamma emission: Often follows alpha or beta decay. The daughter nucleus is in an excited state and releases a gamma photon to drop to its ground state. and unchanged.
Biological effects
Ionising radiation knocks electrons off atoms and breaks chemical bonds. The risk to biological tissue depends on the radiation type and where it lands.
- Alpha is dangerous if ingested or inhaled (a radon decay product in lungs is the classic case) because all energy deposits in a small volume.
- Beta penetrates skin and damages tissue over centimetres.
- Gamma travels through the body; whole-body dose matters.
Carbon-14 undergoes beta-minus decay. Write the balanced equation.
A neutron in carbon-14 becomes a proton, so mass number is unchanged and atomic number rises from to (nitrogen). The emitted beta particle and antineutrino carry away energy and momentum.
- Forgetting the antineutrino in beta-minus decay
- QCAA marking accepts the equation without it for shorter responses, but extended responses should include it.
- Writing change in the wrong direction
- Beta-minus increases (the daughter has one more proton). Beta-plus decreases .
- Calling a gamma emission a "decay"
- Gamma emission is not a decay in the sense of changing the element. It is a transition between energy states of the same nuclide.
- Forgetting that alpha is two protons plus two neutrons
- Some students write the alpha particle as He or He. Always He.
Examples in context
Example 1. Smoke detectors in Brisbane apartments use americium- alpha emitters. The alphas ionise air in a small chamber, sustaining a microcurrent that drops when smoke enters. Alphas (high ionising power, very low penetration) cannot escape the metal cover, so the residential safety case is robust; a sheet of paper or the chamber wall stops them. The same dot-point property table that QCAA Unit 1 students learn is the regulatory basis for ARPANSA's exemption of these devices.
Example 2. Gladstone industrial radiography uses iridium- gamma sources to weld-test pressure vessels. Gammas have low ionising power but high penetration (several centimetres of lead required for half-value shielding). The team enforces a exclusion zone, scaled by the inverse-square law, when activity is . Beta-particle emitters such as strontium- are not used here because they will not penetrate the steel weld. The QCAA EA Unit 1 thematic table maps directly to this industrial choice of isotope.
Try this
Q1. State the charge and approximate mass of an alpha particle and a beta-minus particle. [2 marks]
- Cue. : , ; : , .
Q2. Balance the decay . Identify the daughter and explain why a neutrino is emitted. [3 marks]
- Cue. Daughter ; antineutrino conserves lepton number and energy.
Q3. A radiographer in Gladstone uses an iridium- source. (a) Compare the ionising and penetrating power of gamma to alpha and beta. (b) Justify why gamma is selected. (c) Calculate the activity at from a source treated as a point, using relative to . [3+2+3 marks; ISMG: Knowledge and conceptual understanding, Analysis and interpretation]
- Cue. (a) Gamma: low ionising, high penetration; (b) penetrates steel weld; (c) factor , equivalent.
Exam-style questions
Questions in the style of QCAA exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.
Year 11 SAC-style4 marksUranium-238 (U) undergoes alpha decay. (a) Write the balanced nuclear equation, identifying the daughter nucleus. (b) Compare alpha radiation with gamma radiation in terms of ionising and penetrating power.Show worked answer →
(a) Alpha decay. An alpha particle is . Conservation of mass number and atomic number:
The daughter is thorium-234.
(b) Comparison. Alpha is highly ionising (strong electric charge, low speed, lots of interactions per centimetre travelled) but has low penetration (stopped by a sheet of paper or a few cm of air). Gamma is weakly ionising (no charge, no mass) but highly penetrating (stopped only by thick lead or concrete).
Markers reward conservation of and in the equation, the daughter nucleus identified, and the inverse relationship between ionising power and penetration.