OCR Specification focus:
‘Compare α, β, γ radiation: nature, penetration, range; outline absorption investigations with materials.’
Ionising radiations differ in their physical nature, interactions with matter, and ability to penetrate materials. Understanding these differences is essential for interpreting absorption experiments and explaining how radiation behaves in practical contexts.
The Nature of α, β, and γ Radiation
The three main types of nuclear radiation—alpha (α), beta (β), and gamma (γ)—originate from unstable nuclei undergoing radioactive decay. Each radiation type has distinct physical characteristics that determine how it interacts with matter.
Alpha (α) Radiation
Alpha radiation consists of helium nuclei, each with two protons and two neutrons. Because an α-particle is relatively large and carries a +2 charge, it interacts strongly and frequently with surrounding matter.
These interactions cause α-particles to lose energy rapidly, giving α radiation a very short range in air and high ionising ability.
Alpha radiation: Emission of a helium-4 nucleus containing two protons and two neutrons from an unstable nucleus.
A single sentence helps to separate explanation blocks naturally. Alpha radiation is commonly emitted by heavy, unstable nuclei and is observed in many natural radioactive sources.
Beta (β) Radiation
Beta radiation consists of fast-moving electrons (β⁻) or positrons (β⁺) emitted when a nucleus undergoes a change in quark structure, though the details of quark processes fall outside this subsubtopic. Because β-particles have a much smaller mass than α-particles and carry a single charge, they interact less intensely with matter.
Beta radiation: Emission of high-speed electrons (β⁻) or positrons (β⁺) from an unstable nucleus during radioactive decay.
Beta radiation therefore penetrates further through air and thin materials than α-radiation, although it is less ionising.
Gamma (γ) Radiation
Gamma radiation consists of high-energy photons emitted when a nucleus relaxes from an excited state. Because γ photons have no mass and no charge, they interact only weakly with matter.
Gamma radiation: Emission of high-frequency electromagnetic photons from a nucleus losing excess energy.
Gamma radiation is highly penetrating with a long range in air, though its ionising power is low compared to α and β radiation.
Comparative Penetration and Range
The differences in charge, mass, and energy lead to clear contrasts in how α, β, and γ radiations pass through materials.
Penetration Abilities
Students should be confident in recognising the characteristic penetration patterns:

Diagram comparing how alpha, beta, and gamma radiations are absorbed by paper, aluminium, and lead. Alpha is stopped first, beta penetrates further, and gamma requires thick shielding. Layout is simplified to emphasise qualitative differences. Source.
Alpha radiation
Penetrates only a few centimetres of air.
Stopped by paper or the outer layer of human skin.
Highly ionising due to frequent collisions.
Beta radiation
Penetrates several tens of centimetres of air.
Stopped by a few millimetres of aluminium.
Moderate ionising power.
Gamma radiation
Penetrates many metres of air.
Reduced significantly only by thick lead or several centimetres of dense concrete.
Low ionising power, but potentially hazardous due to long range.
Range in Air
The range of each radiation type can be demonstrated using counter readings:
α: typically 2–5 cm
β: typically up to around 1 m
γ: effectively unlimited for simple laboratory distances, although intensity decreases with distance following an inverse-square relationship.
Absorption Experiments
Absorption experiments provide essential, empirical evidence for the different properties of α, β, and γ radiation. Such experiments often use a Geiger–Müller tube to measure count rates as various materials are placed between the source and the detector.
Basic Experimental Approach
Students should be able to outline how absorption is investigated:
Set up a radioactive source directed towards a Geiger–Müller detector.

Schematic of a Geiger–Müller counter including the end-window tube, high-voltage supply, and counting electronics. The mica window admits low-penetrating radiation while the gas avalanche produces detectable pulses. External absorber sheets are typically placed in front of the window during penetration experiments. Source.
Measure a background count rate and subtract it from all readings to ensure accuracy.
Insert materials of increasing thickness between the source and detector.
Record changes in count rate to determine how each type of radiation is absorbed.
One sentence is included here to ensure spacing between definition and equation blocks, even if no equations are necessary for this topic.
Observations from Absorption Trials
Typical experimental findings include:
Alpha radiation
Detectable only when no absorber or extremely thin materials are present.
Count rate drops to background once even thin paper is inserted.
Beta radiation
Count rate decreases progressively as aluminium sheets increase in thickness.
Little reduction with paper or plastic.
Gamma radiation
Count rate is reduced gradually but never reaches zero, regardless of absorber thickness.
Typical materials such as lead cause only partial attenuation.
Interpreting Results
Absorption experiments help students relate theoretical descriptions of radiation to measurable behaviours. Key interpretations include:
Stronger absorption implies stronger interactions between radiation and matter.
Incomplete absorption, especially for γ radiation, demonstrates the weak interaction of photons with electrons and nuclei.
Sharp drops in count rate, as with α radiation, confirm its short range and high ionising power.
Gradual attenuation curves for γ photons reflect probabilistic interactions described in exponential attenuation relationships, though detailed equations are beyond this subsubtopic.
Practical Considerations in Radiation Studies
Understanding absorption also supports awareness of safe handling practices. Key considerations include:
Using appropriate shielding depending on the radiation type.
Maintaining distance, particularly from γ sources, due to their long range.
Minimising exposure time and using tongs or remote-handling tools.
Monitoring radiation levels frequently during experimental work.
Key Features to Remember
To consolidate understanding of the core conceptual material for this subsubtopic, students should retain the following:
α, β, and γ radiations differ fundamentally in nature, charge, mass, and energy.
These intrinsic properties determine their ionising power, range, and penetration.
Absorption experiments provide essential evidence for comparing these radiations and interpreting their physical behaviours.
FAQ
Alpha particles have a large mass and a +2 charge, causing strong electrostatic interactions with air molecules. These frequent collisions transfer energy rapidly.
Because they ionise many atoms over a short distance, they slow down quickly and are stopped after just a few centimetres. Their short range is therefore a direct consequence of both high charge and high ionising power.
Denser materials contain more nuclei and electrons per unit volume, increasing the probability of interactions.
For beta radiation, dense metals provide more opportunities for scattering and energy loss.
For gamma radiation, dense materials increase the likelihood of photoelectric absorption, Compton scattering, or pair production (although the last is not generally observed in typical school experiments).
Accuracy can be influenced by several controllable variables:
• Distance between source and detector must remain fixed.
• Orientation of the detector window should be consistent.
• Variations in background radiation should be accounted for.
• Source activity may decrease over long periods, although changes are usually negligible in a school setting.
Proper experimental control reduces scatter in count rate data.
Gamma photons interact probabilistically, meaning each photon has a certain chance of being absorbed or scattered.
Thicker shielding increases the probability of interaction but cannot guarantee total absorption unless the material is extremely thick.
As a result, gamma count rates approach background levels asymptotically rather than reaching zero.
Each radiation type interacts through different physical processes:
• Alpha particles cause dense ionisation through direct collisions with electrons.
• Beta particles experience scattering, ionisation, and bremsstrahlung radiation in dense metals.
• Gamma photons interact mainly through photoelectric effect, Compton scattering, or pair production (energy-dependent).
These microscopic interactions collectively produce the macroscopic absorption patterns observed during experiments.
Practice Questions
Question 1 (2 marks)
Alpha, beta, and gamma radiations have different penetrating abilities.
State which type of radiation has:
(a) the shortest range in air
(b) the greatest penetrating power.
Mark scheme:
(a) Alpha radiation (1)
(b) Gamma radiation (1)
Question 2 (5 marks)
A student uses a radioactive source and a Geiger–Müller tube to investigate the absorption of alpha, beta, and gamma radiations.
Describe how the student should carry out this investigation and explain how the results allow the three radiations to be distinguished.
Your answer should include reference to:
• background radiation measurements
• the use of different absorber materials
• expected changes in count rate for each type of radiation.
Mark scheme:
Award marks for any five of the following points:
• Measure background radiation first and subtract it from all readings. (1)
• Place the radioactive source facing the Geiger–Müller tube at a fixed distance. (1)
• Insert different absorber materials of increasing thickness (e.g. paper, aluminium, lead). (1)
• Alpha radiation is stopped by paper or a few centimetres of air, so count rate drops to background immediately. (1)
• Beta radiation is partially absorbed by thin aluminium; count rate falls gradually with thicker aluminium. (1)
• Gamma radiation is only reduced, not fully stopped, even by thick lead; count rate decreases slowly. (1)
