Alpha, beta and gamma radiation

Key idea: Alpha particles ionise most strongly and are stopped by paper. Beta particles travel further and are stopped by a few millimetres of aluminium. Gamma rays ionise least and are only reduced by thick lead.

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Alpha, beta and gamma radiation all come from unstable nuclei, but they behave very differently. A sheet of paper stops alpha particles, while gamma rays pass through a person and need thick lead to cut them down. These differences come from what each radiation is made of, and they help explain applications such as smoke alarms and the different routes by which radiation reaches living tissue.

What alpha, beta and gamma radiation are

RadiationWhat it isWritten asRelative charge
alpha (α)helium nucleus: 2 protons, 2 neutrons⁴₂He+ 2
beta-minus (β⁻)fast-moving electron⁰₋₁e-1
gamma (γ)electromagnetic waveγ0

An alpha particle is relatively massive. A beta-minus particle is an electron, roughly 7000 times lighter than an alpha particle, made in the nucleus when a neutron changes into a proton. A gamma ray has no rest mass and no charge: it is a short-wavelength electromagnetic wave, like light but carrying far more energy.

Check your understanding 1 Separate charge from ionisation

Choose the nature of alpha and beta-minus, then decide whether uncharged gamma radiation can ionise material.

Alpha
Beta-minus
Can gamma radiation ionise material?

Show answer

Alpha is a helium nucleus, beta-minus is an emitted electron from a nuclear process, and gamma is an uncharged photon. Gamma can transfer energy to electrons in matter and cause ionisation. Charge, rest mass and ionising ability are separate properties.

Ionising effect and penetrating power

As radiation passes through a material, it can knock electrons out of the atoms it passes, turning them into ions. This is ionisation. Alpha and beta particles lose energy as they ionise, so dense ionisation gives short tracks. Gamma photons may pass through or interact and transfer energy. A shield reduces the gamma beam’s intensity rather than stopping every photon at one fixed distance.

  • Alpha particles are massive, slow and have a charge of + 2. For typical school examples they produce dense ionisation and lose their energy over a short distance: a few centimetres in air, or a sheet of paper.
  • Beta-minus particles are light, fast and have a charge of -1. Typical beta particles produce less dense ionisation and travel further than typical alpha particles. A few millimetres of aluminium absorbs beta radiation in the examples here; actual range depends on particle energy and the material.
  • Gamma rays have no charge and ionise only weakly, so they are the most penetrating. Thick lead or concrete reduces their intensity, rather than providing a definite stopping thickness for all rays.

So the order of ionising effect is the reverse of the order of penetrating power:

PropertyAlphaBeta-minusGamma
Ionising effectstrongmoderateweak
Penetrating powerlowmoderatehigh
Stopped bypaper, a few cm of aira few mm of aluminiumintensity reduced by thick lead or concrete
Comparing radiation penetrationSeparate alpha, beta-minus and gamma comparisons face paper, aluminium and lead barriers. Alpha ends at paper; beta-minus passes paper and ends at aluminium. Three gamma arrows before lead and one after it illustrate reduced photon transmission without claiming every photon is absorbed. Transmission arrows are not a measured fraction. Actual penetration depends on emission energy and absorber conditions; the drawing is schematic.Typical absorber comparisonsThree separate emission paths; not every source emits all three.Alpha (α)absorbedBeta-minus (β−)absorbedGamma (γ)fewer passPaperThin aluminiumThick leadGamma intensity falls; suitable shielding does not guarantee zero transmission.
Comparing radiation penetrationSeparate alpha, beta-minus and gamma comparisons face paper, aluminium and lead barriers. Alpha ends at paper; beta-minus passes paper and ends at aluminium. Three gamma arrows before lead and one after it illustrate reduced photon transmission without claiming every photon is absorbed. Transmission arrows are not a measured fraction. Actual penetration depends on emission energy and absorber conditions; the drawing is schematic.Typical absorber comparisonsThree separate emission paths; not every source emits all three.Alpha (α)absorbedBeta-minus (β−)absorbedGamma (γ)fewer passPaperThin aluminiumThick leadGamma intensity falls; suitable shielding does not guarantee zero transmission.
Typically, paper stops alpha, suitable aluminium stops beta-minus, and thick lead reduces gamma intensity. Fewer gamma arrows mean fewer transmitted photons, not slower photons.

Worked example 1

Identifying radiation with a sheet of paper

Problem

A detector near a source gives a count-rate well above background. When a sheet of paper is placed between the source and the detector, the count-rate falls to the background level. For this idealised identification question, the detector is sensitive to all three radiation types and the readings are repeated at fixed geometry. Which radiation best fits the paper test? Explain what a background-level reading tells you.

Show full solution
  1. Use the absorber

    Method

    The detected source contribution is consistent with alpha radiation; no remaining source contribution is resolved after the paper.

    Reason

    Paper stops alpha particles. A detectable beta or gamma contribution would remain above background in the stated model. A weak beta or gamma contribution could be too small to detect above the background fluctuations.

    Working

    Answer

    Stopped by paper → alpha.

  2. Link to ionisation

    Method

    Alpha particles are stopped so easily because they ionise so strongly.

    Reason

    They give up their energy in many ionisations over a very short distance.

    Working

    Answer

    Strong ionisation → rapid energy loss → short range.

Exam-style question 1

Choosing an absorber for beta radiation

2 marks

Examination question

A source emits beta-minus radiation only. Which of these would stop the radiation: a sheet of paper, a few millimetres of aluminium, or a few centimetres of air? Explain your answer. [2 marks]

Choose the absorber and its penetration reason

Absorber in the stated school example
Reason

Show full solution
  1. Choose and explain

    2 marks

    Method

    A few millimetres of aluminium.

    Reason

    Beta-minus particles are more penetrating than alpha particles, so they pass through paper, but they are stopped by a few millimetres of aluminium.

    Working

    Answer

    Paper: not enough. Aluminium, a few mm: stops beta.

Check your understanding 2 Can gamma rays ionise?

A learner says, “Gamma rays have no charge, so they cannot ionise anything.” Explain the energy transfer that makes this possible, on paper or here. Compare your full explanation below; a typed note is optional.

Show answer

Gamma photons carry energy and can transfer enough to remove an electron from an atom. They ionise less densely than typical alpha or beta particles because their interactions are less frequent; many photons can pass through substantial thicknesses of material.

Try it yourself 1

Reading a cloud chamber track

Minimal support

Problem

In a cloud chamber, tiny droplets form on the ions left behind by a particle, so the particle’s path shows up as a track. One source produces short, thick, straight tracks. Which radiation is it most likely to be? Explain both features of the tracks.

Interpret thickness, then length, then likely identity

Thick track suggests
Short track suggests
Most likely of alpha, beta-minus or gamma

Hints

Hint 1

thickness

A thick track means many droplets, so many ions were made along the path.

Hint 2

length

A radiation that ionises strongly uses up its energy over a short distance.

Show solution step by step
  1. Thick tracks

    Method

    The radiation ionises strongly.

    Reason

    Many ions along the path give many droplets, so the track is thick.

    Working

    Answer

    Thick track → strong ionisation.

  2. Short tracks

    Method

    The radiation is alpha.

    Reason

    Strong ionisation uses up the particle’s energy within a few centimetres of air, so the track is short.

    Working

    Answer

    Short, thick track → alpha.

Which radiation is most dangerous?

Penetration and ionisation matter together with the exposure route. Alpha radiation is largely stopped by intact outer skin, while penetrating gamma radiation can reach internal tissue from outside. Alpha-emitting material inside the body can deposit energy densely in nearby living tissue. This does not rank every source: risk also depends on activity, radiation energy, exposure time and where radioactive material goes in the body. See the EPA explanation of exposure pathways and radiation risk.

Spot the mistake 1

Is alpha always the most dangerous?

About 5 min

Learner response

A learner says, “Alpha is the most ionising, so an alpha source on a laboratory bench is always more dangerous to stand near than a gamma source.” Correct the learner.

Compare access to living tissue before ranking danger

Is the claim always valid?
Most penetrating radiation towards deep organs from outside
Why internal alpha emitters can be harmful

Show solution step by step
  1. The alpha source outside the body

    Method

    Alpha particles from the bench are stopped by a few centimetres of air or by the outer layer of skin.

    Reason

    Their strong ionisation gives them a very short range, so they do not generally reach internal tissue through intact skin.

    Working

    Answer

    External alpha through intact skin: strongly ionising but limited penetration.

  2. The gamma source outside the body

    Method

    Gamma rays can reach internal organs from outside the body.

    Reason

    They are penetrating enough to pass through the skin and reach internal organs, where they can ionise.

    Working

    Answer

    External gamma: weakly ionising but reaches the organs.

Deflection in an electric field

Because alpha and beta-minus particles are charged, they are deflected when they pass between charged plates. Alpha particles, being positive, bend towards the negative plate. Beta-minus particles, being negative, bend towards the positive plate. Gamma rays have no charge and go straight on. The direction follows charge sign. The amount of bending also depends on speed, field strength and time in the field; the figure illustrates directions rather than giving a universal curvature ratio.

Radiation in an electric fieldA positive upper plate and negative lower plate create a downward electric field. Alpha moving right curves gently downward, beta-minus moving right curves sharply upward, and gamma travels straight. Arrows distinguish beam motion from electric-field direction. Charge sign sets deflection direction; bend size also depends on charge magnitude, mass, speed, field strength and time in the field. Curves are illustrative, not measured.Direction follows charge signBeams enter moving from left to right.Positive plate (+)Negative plate (−)electric fieldBeta (−1)bends sharply, toward +Gamma (0)straightAlpha (+2)bends a little, toward −Direction follows charge sign; mass, speed and field affect bend size.
Radiation in an electric fieldA positive upper plate and negative lower plate create a downward electric field. Alpha moving right curves gently downward, beta-minus moving right curves sharply upward, and gamma travels straight. Arrows distinguish beam motion from electric-field direction. Charge sign sets deflection direction; bend size also depends on charge magnitude, mass, speed, field strength and time in the field. Curves are illustrative, not measured.Direction follows charge signBeams enter moving from left to right.Positive plate (+)Negative plate (−)electric fieldBeta (−1)bends sharply, toward +Gamma (0)straightAlpha (+2)bends a little, toward −Direction follows charge sign; mass, speed and field affect bend size.
Alpha bends towards the negative plate, beta-minus towards the positive plate, and gamma stays straight. The curves are illustrative, not to scale.

Guided practice 1

Identifying radiation by its deflection

About 4 min

Problem

A narrow beam of radiation passes between two charged plates and bends towards the positive plate. Identify the radiation and state its charge.

Work out the sign of the charge first

Radiation

Hints

Hint 1

attraction

Opposite charges attract. What sign of charge is pulled towards a positive plate?

Hint 2

identity

Which of the three radiations has a negative charge?

Show solution step by step
  1. Find the sign of the charge

    Method

    The radiation is negatively charged.

    Reason

    It is attracted towards the positive plate.

    Working

    Answer

    Bends towards + → negative charge.

  2. Identify it

    Method

    Beta-minus radiation, with a charge of -1.

    Reason

    It is the only negatively charged one of the three.

    Working

    Answer

    β⁻ = ⁰₋₁e

Check your understanding 3 Reverse the field and reconstruct the paths

On paper, draw three beams entering from left to right between an upper negative plate and lower positive plate. Show the electric field and the initial bending direction of alpha and beta-minus, then gamma’s path. Explain the charge-to-force link for each; no numerical curvature is required. Compare the complete labelled sketch below; a typed note is optional.

Show answer

The electric field points upwards, from the lower positive plate to the upper negative plate. Alpha has +2 charge, so its force and initial bending are upwards towards the negative plate. Beta-minus has −1 charge, so its force and initial bending are downwards towards the positive plate. Gamma is uncharged and continues straight in this electric field. Check both plate signs, beam-motion arrows, the field arrow and all three paths with their charge reasons. The sketch does not assign measured bending angles or uniquely identify a source from one track.

Common mistakes

  • Mixing up the two orders. Alpha ionises most and penetrates least; gamma ionises least and penetrates most.
  • Saying gamma rays are charged, or that they cannot ionise at all.
  • Saying alpha radiation is harmless. It is very dangerous inside the body.
  • Saying a sheet of lead stops all gamma rays. Lead reduces their intensity; thicker lead reduces it more.
  • Saying a beta-minus particle is an electron from the atom’s outer shells. It is made in the nucleus.
  • Expecting a detector reading to fall to zero when the source contribution is absorbed. It approaches the background reading, which fluctuates.

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