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A Level Physics 9702 · AS Level · Topic 11 · ~7 min read

Particle physics

What α-particle scattering tells us about the nucleus, nuclide notation and isotopes, α, β⁻, β⁺ and γ radiation, antiparticles and neutrinos, decay equations, and quarks, hadrons and leptons with the quark changes in β decay.

α-particle scatteringNuclear modelNucleon & proton numberIsotopesα, β⁻, β⁺, γAntiparticlesNeutrinosDecay equations
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Paper tag = where it is examinedDATA & FORMULAE given in the examC1A1B1 how marks are awardedhighlight = comes up again and againTest yourself at the end

In 30 seconds

  • α-particle scattering showed that an atom's positive charge and almost all its mass are concentrated in a tiny nucleus.
  • Nuclide notation AZX: A = nucleon number (protons + neutrons), Z = proton number. Isotopes have the same Z but different numbers of neutrons.
  • In every nuclear process nucleon number and charge are conserved.
  • β⁻ decay emits an electron and an electron antineutrino (a neutron becomes a proton: d → u). β⁺ decay emits a positron and an electron neutrino (u → d).
  • Quarks (up, down, strange, charm, top, bottom) are fundamental. Baryons are three quarks; mesons are a quark and an antiquark. Electrons and neutrinos are leptons, also fundamental.

By the end you can

  • Infer the size and nature of the nucleus from α-particle scattering.
  • Use nuclide notation and the terms nucleon number, proton number and isotope.
  • Describe α, β⁻, β⁺ and γ radiation and write balanced decay equations.
  • Explain antiparticles, and why β-particles have a continuous energy spectrum.
  • Describe protons and neutrons in terms of quarks and the quark changes in β decay.

1The nuclear atom

α-particle scattering

gold nucleusmost α pass straight through (blue)a few deflected (orange); about 1 in 8000 bounce back (red): a tiny, dense, positive nucleus
Most α-particles pass straight through; a few are deflected; a very few bounce back.
ObservationInference
Most α-particles pass straight through the gold foilmost of the atom is empty space
A few are deflected through small anglesthere is a concentration of positive charge that repels them
A very small fraction (about 1 in 8000) are deflected by more than 90°the positive charge and most of the mass are concentrated in a very small, dense nucleus
  • The simple nuclear model: a tiny nucleus (diameter about 10⁻¹⁵ to 10⁻¹⁴ m) of protons and neutrons, surrounded by orbital electrons (atom diameter about 10⁻¹⁰ m).

Nuclides and isotopes

Nucleon number (A) — the total number of protons and neutrons in a nucleus.

Proton number (Z) — the number of protons in a nucleus.

Isotopes — nuclides of the same element (same proton number) with different numbers of neutrons.

  • Example: 5626Fe has 26 protons and 56 − 26 = 30 neutrons; a neutral atom also has 26 electrons.
  • Unified atomic mass unit: 1 u = 1.66 × 10⁻²⁷ kg (one-twelfth of the mass of a carbon-12 atom). A proton or neutron is about 1 u.
Common mistakePutting the nucleon and proton numbers the wrong way round, or writing the neutron number as the nucleon number. Both were 2024 Paper 2 errors.

2Radiation and decay

α, β and γ

RadiationCompositionChargeMassTypical speed
αhelium nucleus, 2 protons + 2 neutrons+2e4 uabout 0.05c
β⁻electron−e1/1840 uup to about 0.99c
β⁺positron (antielectron)+e1/1840 uup to about 0.99c
γelectromagnetic radiation (photon)00c

Antiparticle — a particle with the same mass as its corresponding particle but opposite charge (and other opposite quantum numbers). The positron is the antiparticle of the electron.

Decay equations

  • Balance both rows: the top numbers (nucleon number) and the bottom numbers (charge/proton number) must add up on each side.
23892U → 23490Th + 42α
α decay: A − 4, Z − 2
146C → 147N + 0−1e + ν̄
β⁻ decay: A unchanged, Z + 1, an electron antineutrino is emitted
²²₁₁Na → ²²₁₀Ne + ⁰₊₁e + ν
β⁺ decay: A unchanged, Z − 1, an electron neutrino is emitted
  • γ emission changes neither A nor Z; the nucleus loses energy (often just after α or β decay).

Energy spectra

β kinetic energynumberEmaxA continuous spread: the missing energy is carried by a neutrino.
β-particles have a continuous range of kinetic energies up to a maximum.
  • α-particles from one nuclide have discrete (fixed) energies, because the decay produces only two products, which share the energy in a fixed way.
  • β-particles have a continuous range of energies, because a third particle (the antineutrino or neutrino) is emitted and shares the released energy in varying proportions.
Common mistakeDescribing β energies as discrete, or describing the continuous spectrum without saying that another particle (the (anti)neutrino) must be emitted. Both lost marks in 2024 Paper 2.

3Fundamental particles

Quarks

QuarkSymbolCharge
upu+⅔e
downd−⅓e
stranges−⅓e
charmc+⅔e
topt+⅔e
bottomb−⅓e
  • Antiquarks (ū, d̄, …) have the opposite charge: ū is −⅔e, d̄ is +⅓e.
  • Hadrons are made of quarks: a baryon has three quarks (proton uud, neutron udd); a meson has a quark and an antiquark (e.g. π⁺ = ud̄, charge +⅔ + ⅓ = +1).
  • Leptons are fundamental and are not made of quarks: electrons, positrons and neutrinos.
uudproton: uud, +⅔ +⅔ −⅓ = +1uddneutron: udd, +⅔ −⅓ −⅓ = 0β⁻ decay:d → u + e⁻ + ν̄(neutron → proton)β⁺ decay:u → d + e⁺ + ν(proton → neutron)Quark charges: u, c, t = +⅔e; d, s, b = −⅓e. Antiquarks have the opposite charge.Meson = quark + antiquark (e.g. π⁺ = u d̄). Baryon = three quarks.
Protons and neutrons are not fundamental; their charges come from their quarks.

Quark changes in β decay

  • β⁻: a neutron becomes a proton: udd → uud, so one d quark changes to a u quark: d → u + e⁻ + ν̄.
  • β⁺: a proton becomes a neutron: uud → udd, so one u quark changes to a d quark: u → d + e⁺ + ν.
  • Check the charge: d (−⅓) → u (+⅔) + e⁻ (−1) + ν̄ (0): −⅓ = +⅔ − 1 ✓.
Common mistakeSwapping β⁺ and β⁻ (2024 Paper 1). β⁻: neutron → proton, electron and antineutrino. β⁺: proton → neutron, positron and neutrino.
Linking questionMass–energy and binding energy explain why nuclei decay in Nuclear physics; positrons annihilate with electrons in PET scanning in Medical physics; and charge quantisation links to Electricity.

Test yourself — cover the answers first

Quick check

  1. State one conclusion from the fact that most α-particles pass straight through gold foil.
  2. How many neutrons are in 23592U?
  3. Which particle is emitted with the electron in β⁻ decay?
  4. What is the quark composition of a neutron?
  5. What is the charge of a meson made of s and ū?

Exam-style

  1. Polonium-210 (Z = 84) emits an α-particle. Write the decay equation and name the daughter's proton number.
  2. Explain why the energy of β-particles from a sample is continuous, while α-particles have discrete energies.
  3. A particle consists of an up quark and an anti-down quark. State whether it is a baryon or meson and find its charge.
Show answers
  1. most of the atom is empty space
  2. 143
  3. an electron antineutrino
  4. udd
  5. −⅓ − ⅔ = −1 (e)
  6. 21084Po → 20682Pb + 42α; Z = 82
  7. β decay produces three particles (daughter, β, (anti)neutrino) sharing the energy in variable proportions; α decay has two products with fixed shares
  8. meson; +⅔ + ⅓ = +1e
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Independent notes written by Riyaz Sir. Not produced, endorsed or approved by Cambridge University Press & Assessment. Syllabus codes 9709 and 9702 refer to the Cambridge International AS & A Level syllabuses.