Revision Notes
OxfordAQA International AS and A-level Physics: Atomic structure and elementary particles (9630) – Revision Notes
Condensed recall notes and a self-test on atomic structure, specific charge, nuclide notation and antiparticles for OxfordAQA International Physics 9630.
- Subject
- Physics
- Level
- AS LEVEL
- Topic
- Atomic structure and elementary particles
- Author
- Marlbridge Academic Team
- Updated
Aligned to OxfordAQA A Level Physics (9630), International AS and A-level. Official specification .
Syllabus page (what it covers and how it is assessed): OxfordAQA A Level Physics.
Syllabus points this page covers
9630 (AS Level)
- 3.3.1 Constituents of the atom
- 3.3.2 Elementary particles
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Need help with this topic? Request a free trial class for A Level Physics (9630).
These are condensed notes for the final weeks on sections 3.3.1 and 3.3.2 of the OxfordAQA International AS and A-level Physics (9630) specification, Version 4.4. Both sections are shared International AS and A-level content. For full explanations and worked examples, read the study guide, then test yourself with the practice set.
Related pages: physics hub, printable checklist and the free 10-minute diagnostics. The atomic mass unit is not required at International AS (it is in section 3.12.2, International A-level), so keep masses in kg or in relative units.
3.3.1 Constituents of the atom
Simple model. A small, dense, positive nucleus (protons and neutrons, called nucleons) surrounded by electrons. A neutral atom has Z electrons.
Scale. Atomic radii are about 10⁻¹⁰ m; nuclear radii are about 10⁻¹⁵ m. Nearly all the mass is in the nucleus.
Rutherford scattering in one box
| Set-up | Why |
|---|---|
| Alpha source, thin gold foil, detector that moves round | Count alpha particles at different angles |
| Vacuum | Air would absorb or scatter alpha particles |
| Very thin foil | Each alpha particle scatters at most once |
| Result | Meaning |
|---|---|
| Most pass straight through | The atom is largely empty space |
| Few deflected through large angles | Small concentrated positive charge (repulsion) |
| Very few rebound | Nucleus is massive as well as positive |
How the model changed
- Positive charge spread through the atom with electrons embedded (“plum pudding”). This predicts only small deflections.
- Scattering evidence led to the nuclear atom.
- The neutron was identified in 1932, explaining why nuclear mass exceeds what the proton count suggests.
- Protons and neutrons are now known to have internal structure (not needed for this section).
Key idea: a model stays until evidence contradicts it.
Properties table
| Particle | Relative charge | Relative mass | Charge (C) | Mass (kg) |
|---|---|---|---|---|
| Proton | +1 | 1 | +1.60 × 10⁻¹⁹ | 1.67 × 10⁻²⁷ |
| Neutron | 0 | 1 | 0 | 1.67 × 10⁻²⁷ |
| Electron | −1 | about 1/1840 | −1.60 × 10⁻¹⁹ | 9.11 × 10⁻³¹ |
Nuclide notation
A
X A = nucleon number (protons + neutrons)
Z Z = proton number
Neutrons = A − Z. Electrons in a neutral atom = Z. Isotopes: same Z, different A.
Specific charge
specific charge = charge / mass, in C kg⁻¹.
Method in steps:
- Find the net charge: (protons − electrons) × 1.60 × 10⁻¹⁹ C. For a bare nucleus, use Z protons only.
- Find the mass: A × 1.67 × 10⁻²⁷ kg (ignore electrons unless the question gives their mass).
- Divide, keep the sign, give units and 3 significant figures.
Reference values: proton 9.58 × 10⁷ C kg⁻¹. Electron 1.76 × 10¹¹ C kg⁻¹.
Quick check: a nucleus with Z protons and A nucleons has specific charge Z/A times the proton value. For helium-4 that is 2/4, so half the proton value.
3.3.2 Elementary particles
For every type of particle there is a corresponding antiparticle. Know these four pairs:
| Particle | Antiparticle | Charge | Rest energy (MeV) |
|---|---|---|---|
| Electron | Positron | opposite | 0.511 for both |
| Proton | Antiproton | opposite | 938.3 for both |
| Neutron | Antineutron | both 0 | 939.6 for both |
| Neutrino | Antineutrino | both 0 | negligible at this level |
Must-know distinction. A particle and its antiparticle share mass and rest energy but carry opposite charge. Neutral particles still have distinct antiparticles.
E = mc² is not required in calculations. Use rest energies in MeV. Convert: 1 MeV = 1.60 × 10⁻¹³ J.
Annihilation
A particle and its antiparticle vanish together, and photons carry off the energy. Charge, energy and momentum are conserved. At least two photons, in opposite directions.
Energy of photons = both rest energies + both kinetic energies.
Example: electron and positron at rest give two photons of 0.511 MeV each (1.022 MeV in total).
Pair production
Photon becomes particle + antiparticle, near a nucleus. Minimum photon energy = twice the rest energy of one particle.
| Pair | Minimum photon energy |
|---|---|
| Electron and positron | 1.022 MeV |
| Proton and antiproton | 1876.6 MeV |
Extra energy becomes kinetic energy of the pair.
Method in steps for energy questions
- Write the rest energy of each particle in MeV.
- Add kinetic energy for annihilation, or subtract the rest energies from the photon energy for pair production.
- Divide by two if the two products share energy equally (symmetrical case).
- Convert to joules only if asked.
Worked reminders
Ion. Find the specific charge of the magnesium ion with 12 protons, 12 neutrons and 10 electrons.
- Net charge = (12 − 10)e = +2e = 3.20 × 10⁻¹⁹ C.
- Nucleon number = 24, so mass ≈ 24 × 1.67 × 10⁻²⁷ = 4.01 × 10⁻²⁶ kg.
- Specific charge = 3.20 × 10⁻¹⁹ ÷ 4.01 × 10⁻²⁶ = 7.98 × 10⁶ C kg⁻¹.
Annihilation. An electron and a positron, each with 0.30 MeV of kinetic energy, meet head-on.
- Each has 0.511 + 0.30 = 0.811 MeV.
- Total = 1.622 MeV, shared by two photons.
- Each photon: 0.811 MeV, or 0.811 × 1.60 × 10⁻¹³ = 1.30 × 10⁻¹³ J.
Pair production check. A photon must carry at least 1.022 MeV. If it has 2.022 MeV, the pair shares 1.000 MeV of kinetic energy.
Writing a Rutherford answer
A full answer has three linked parts: the observation, the physics, and the conclusion.
- Observation: “A small number of alpha particles were deflected through large angles.”
- Physics: “Alpha particles are positive and are repelled by a positive charge.”
- Conclusion: “The positive charge must be concentrated in a very small region, the nucleus.”
Do the same for the other two observations in the table, and always mention that the experiment was done in a vacuum with a thin foil.
Quick links between ideas
- The specific charge of a nucleus is Z/A times that of a proton. Isotopes of one element therefore have slightly different specific charges, because A differs while Z is fixed.
- Particle and antiparticle rest energies are equal, so the pair-production threshold is always twice one rest energy.
- A neutral atom has no overall charge. An ion has a net charge, so its specific charge is not zero.
Quick self-test
- How many neutrons are in the nucleus of uranium-238, which has proton number 92?
- How many protons, neutrons and electrons does a 39K⁺ ion contain (proton number 19).
- Calculate the specific charge of the lithium-7 nucleus (proton number 3), giving units.
- State the relative charge and approximate relative mass of an electron.
- What is the minimum photon energy needed to produce a proton and an antiproton?
- Why must at least two photons be produced when a stationary electron and positron annihilate?
- A photon of energy 1.50 MeV produces an electron-positron pair. Find the kinetic energy of each, assuming they share it equally.
- Give the antiparticle of the neutrino, and state its charge.
- Convert a photon energy of 2.40 MeV to joules.
- Explain why a photon of energy 0.90 MeV cannot produce an electron-positron pair.
- Which observation in the scattering experiment shows that the target is more massive than the alpha particles?
- Why was the foil in the scattering experiment very thin?
Answers
- 238 − 92 = 146 neutrons.
- Nucleon number 39, so neutrons = 20. Electrons = 19 − 1 = 18. 19 protons, 20 neutrons, 18 electrons.
- Three protons carry 4.80 × 10⁻¹⁹ C in total. Mass ≈ 7 × 1.67 × 10⁻²⁷ = 1.17 × 10⁻²⁶ kg. Specific charge = 4.11 × 10⁷ C kg⁻¹.
- Relative charge −1; relative mass about 1/1840.
- 2 × 938.3 = 1876.6 MeV.
- Momentum must be conserved. The total momentum before is zero, and one photon carries momentum, so there must be at least two, moving in opposite directions.
- Available = 1.50 − 1.022 = 0.478 MeV; each gets 0.239 MeV.
- The antineutrino, with zero charge.
- 2.40 × 1.60 × 10⁻¹³ = 3.84 × 10⁻¹³ J.
- The minimum energy is 1.022 MeV, and 0.90 MeV is less than this, so there is not enough energy to create two particles of rest energy 0.511 MeV each.
- The small number of alpha particles that rebounded through angles above 90 degrees.
- So each alpha particle is scattered by at most one nucleus and few are absorbed.
Where marks are usually lost
- Giving the neutron count as A instead of A − Z.
- Leaving out the negative sign on the specific charge of a negative ion or the electron.
- Using Z protons for the charge of an ion instead of the net charge.
- Stating only “most of the atom is empty space” for Rutherford. Write each observation with its own conclusion.
- Saying “attraction” instead of repulsion between the nucleus and the alpha particles.
- Using a single rest energy as the pair-production threshold.
- Mixing MeV and joules in one calculation.
- Writing that antimatter has negative mass or that the neutron and antineutron are identical.
Official syllabus
OxfordAQA International AS and A-level Physics (9630), sections 3.3.1 and 3.3.2, Version 4.4 (for exams May/June 2020 onwards), published by OxfordAQA.
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Original practice questions with worked answers on Rutherford scattering, specific charge, antiparticles, annihilation and pair production.
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