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Alpha, beta and gamma radiation (QCE Physics Unit 1)

Syllabus dot point

“Describe the properties of alpha, beta and gamma radiation, including charge, mass, ionising and penetrating power, and represent decay reactions using balanced nuclear equations”

8 min read

Quick answer

Alpha radiation is a 24^4_2He nucleus (charge +2+2, very strongly ionising, stopped by paper); beta-minus is a high-speed electron (charge −1-1, 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 AA and atomic number ZZ.

Jump to a section
  1. What this dot point is asking
  2. The three types
  3. Why ionising power and penetration are inverse
  4. Balanced nuclear equations
  5. Biological effects
  6. Examples in context
  7. Try this
  8. Exam-style questions

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 α\alpha or 24He^4_2\text{He} 22 protons, 22 neutrons +2+2 44 ∼0.1c\sim 0.1c at most Very strong Very low Sheet of paper, ∼\sim cm of air
Beta-minus β−\beta^- or −10e^0_{-1}e high-speed electron −1-1 ∼1/1836\sim 1/1836 up to ∼0.99c\sim 0.99c Moderate Moderate Few mm of aluminium
Gamma γ\gamma high-energy photon 00 00 cc Weak Very high Thick lead or concrete

Beta-plus (β+\beta^+, 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 AA (total number of nucleons),
  • atomic number ZZ (total charge).

Alpha decay: AA drops by 44, ZZ drops by 22.

ZAX→Z−2A−4Y+24He^A_Z X \to ^{A-4}_{Z-2} Y + ^4_2 \text{He}

Beta-minus decay: A neutron becomes a proton plus an electron plus an antineutrino. AA unchanged, ZZ increases by 11.

ZAX→Z+1AY+−10e+νˉe^A_Z X \to ^{A}_{Z+1} Y + ^0_{-1} e + \bar{\nu}_e

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. AA and ZZ unchanged.

ZAY∗→ZAY+γ^A_Z Y^* \to ^A_Z Y + \gamma

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.
Worked example

Carbon-14 undergoes beta-minus decay. Write the balanced equation.

614C→714N+−10e+νˉe^{14}_{6}\text{C} \to ^{14}_{7}\text{N} + ^0_{-1} e + \bar{\nu}_e

A neutron in carbon-14 becomes a proton, so mass number 1414 is unchanged and atomic number rises from 66 to 77 (nitrogen). The emitted beta particle and antineutrino carry away energy and momentum.

Common traps
Forgetting the antineutrino in beta-minus decay
QCAA marking accepts the equation without it for shorter responses, but extended responses should include it.
Writing ZZ change in the wrong direction
Beta-minus increases ZZ (the daughter has one more proton). Beta-plus decreases ZZ.
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 44^4_4He or 14^4_1He. Always 24^4_2He.

Examples in context

Example 1. Smoke detectors in Brisbane apartments use americium-241241 alpha emitters. The 5.5 MeV5.5 \text{ MeV} 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-192192 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 30 m30 \text{ m} exclusion zone, scaled by the inverse-square law, when activity is 300 GBq300 \text{ GBq}. Beta-particle emitters such as strontium-9090 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. α\alpha: +2e+2e, 4.00 u4.00 \text{ u}; β−\beta^-: −e-e, 5.5×10−4 u5.5 \times 10^{-4} \text{ u}.

Q2. Balance the decay 614C→?+β−+νˉe^{14}_{6}\text{C} \rightarrow ? + \beta^- + \bar{\nu}_e. Identify the daughter and explain why a neutrino is emitted. [3 marks]

  • Cue. Daughter 714N^{14}_{7}\text{N}; antineutrino conserves lepton number and energy.

Q3. A radiographer in Gladstone uses an iridium-192192 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 7 m7 \text{ m} from a 300 GBq300 \text{ GBq} source treated as a point, using I∝1/r2I \propto 1/r^2 relative to 1 m1 \text{ m}. [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 1/491/49, 6.1 GBq6.1 \text{ GBq} 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 marks
Uranium-238 (92238^{238}_{92}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 24He^{4}_{2}\text{He}. Conservation of mass number and atomic number:

92238U→90234Th+24He^{238}_{92}\text{U} \to ^{234}_{90}\text{Th} + ^{4}_{2}\text{He}

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 AA and ZZ in the equation, the daughter nucleus identified, and the inverse relationship between ionising power and penetration.

Practise this

Sources & how we know this

ExamExplained