β Unit 1: Thermal, nuclear and electrical physics
Topic 2: Ionising radiation and nuclear reactions
Describe the properties of alpha, beta and gamma radiation, including charge, mass, ionising and penetrating power, and represent decay reactions using balanced nuclear equations
A focused answer to the QCE Physics Unit 1 dot point on the three common types of ionising radiation. Tabulates the charge, mass, ionising power, penetration and shielding of alpha, beta and gamma radiation, and works the QCAA-style balanced-nuclear-equation problem that appears in EA Paper 1.
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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 | IMATH_3 or IMATH_4 | IMATH_5 protons, neutrons | IMATH_7 | IMATH_8 | IMATH_9 at most | Very strong | Very low | Sheet of paper, cm of air |
| Beta-minus | IMATH_11 or IMATH_12 | high-speed electron | IMATH_13 | IMATH_14 | up to IMATH_15 | Moderate | Moderate | Few mm of aluminium |
| Gamma | IMATH_16 | high-energy photon | IMATH_17 | IMATH_18 | IMATH_19 | 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.
Worked example
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.
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 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.
In one sentence
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 .
Past exam questions, worked
Real questions from past QCAA papers on this dot point, with our answer explainer.
Year 11 SAC4 marksUranium-238 ($^{238}_{92}$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 β
(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.
Related dot points
- Solve problems involving the exponential decay of radioactive nuclides, half-life and decay constant, and apply to radiometric dating and medical applications
A focused answer to the QCE Physics Unit 1 dot point on half-life and radioactive decay. Applies $N = N_0 (1/2)^{t/T_{1/2}}$ and the decay constant $\lambda = \ln 2 / T_{1/2}$, walks through radiometric dating (carbon-14) and medical applications (technetium-99m), and works the QCAA-style number-of-half-lives problem.
- Describe nuclear fission and nuclear fusion, including the role of binding energy per nucleon, and apply mass-energy equivalence ($E = mc^2$) to estimate the energy released
A focused answer to the QCE Physics Unit 1 dot point on fission and fusion. Reads the binding-energy curve to show why both reactions release energy, applies $E = mc^2$ to mass defect, and works the QCAA-style energy-per-reaction problem from EA Paper 2 with worked U-235 numbers.
- Atomic nucleus, isotopes, types of radioactive decay (alpha, beta, gamma), half-life, fission and fusion
A focused answer to the QCE Physics Unit 1 subject-matter point on nuclear physics. Atomic structure, isotopes, alpha/beta/gamma decay, half-life formula $N = N_0(1/2)^{t/T_{1/2}}$, fission and fusion.