← Unit 1: Thermal, nuclear and electrical physics

QLDPhysicsSyllabus dot point

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.

Generated by Claude OpusReviewed by Better Tuition Academy6 min answer

Have a quick question? Jump to the Q&A page

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, 22 neutrons IMATH_7 IMATH_8 IMATH_9 at most Very strong Very low Sheet of paper, ∼\sim 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 (Ξ²+\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.

ZAXβ†’Zβˆ’2Aβˆ’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.

ZAXβ†’Z+1AY+βˆ’10e+Ξ½Λ‰e^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.

ZAYβˆ—β†’ZAY+Ξ³^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.

614Cβ†’714N+βˆ’10e+Ξ½Λ‰e^{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.

In one sentence

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 βˆ’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.

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 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.

Related dot points