An atom has a tiny, dense nucleus of protons and neutrons, surrounded by orbiting electrons.
A nuclide is written AZX, where A is the nucleon number and Z the proton number; the neutron number is N = A − Z.
Specific charge is the charge-to-mass ratio of a particle:
The electron has the largest specific charge (small mass); the neutron's is zero (no charge).
Find the specific charge of a proton (charge 1.6×10−19 C, mass 1.673×10−27 kg).
Isotopes have the same proton number but different neutron numbers; they are chemically identical.
An ion forms when an atom gains or loses electrons, giving it a net negative or positive charge (a multiple of 1.6×10−19 C).
Chlorine's relative atomic mass of 35.5 arises from a mixture of 3517Cl (about 75%) and 3717Cl (about 25%).
Electromagnetic radiation is emitted in packets (photons) of energy:
The electronvolt (eV) is the energy transferred when an electron moves through a p.d. of 1 V: 1 eV = 1.6×10−19 J.
Calculate the energy of a photon of frequency 5.0×1014 Hz (h = 6.63×10−34 J s).
Every particle has a corresponding antiparticle with the same mass and rest energy but opposite charge, baryon number, lepton number and strangeness.
When a particle meets its antiparticle they annihilate, converting their total rest energy into two gamma photons.
The pair approach with equal and opposite momenta, so the total momentum beforehand is zero. The two photons must therefore travel in exactly opposite directions — which is why two photons are produced and never one.
The energy locked up in a particle's mass is its rest energy, given by Einstein's mass–energy equation:
Calculate the rest energy of an electron (mass 9.11×10−31 kg) in J and in MeV.
Pair production is the reverse of annihilation: a high-energy photon creates a particle-antiparticle pair, usually near a nucleus (which recoils to conserve momentum).
The photon must have at least the total rest energy of the pair: Emin = 2 m c2.
The three quarks at A-level are up (u), down (d) and strange (s). Antiquarks have the opposite sign of charge, baryon number and strangeness.
A baryon is three quarks (qqq). The two you must know are the proton and the neutron:
Quarks carry fractional charges, but no free particle has ever been observed with a fractional charge. Every baryon and every meson must therefore have a whole-number charge — 0, ±1e or ±2e. This is a useful check: if a proposed combination of quarks does not come to an integer, it cannot be a real hadron.
The properties of the quarks are given to you in the exam:
| Quark | Charge | Baryon No. | Strangeness | Charmness | Bottomness | Topness |
|---|---|---|---|---|---|---|
| d | −⅓ | +⅓ | 0 | 0 | 0 | 0 |
| u | +⅔ | +⅓ | 0 | 0 | 0 | 0 |
| s | −⅓ | +⅓ | −1 | 0 | 0 | 0 |
| c | +⅔ | +⅓ | 0 | +1 | 0 | 0 |
| b | −⅓ | +⅓ | 0 | 0 | −1 | 0 |
| t | +⅔ | +⅓ | 0 | 0 | 0 | +1 |
All hadrons feel the strong interaction and are made of quarks. They come in exactly two kinds:
A meson is always one quark and one antiquark (qq̅). The two families you need are the pions and the kaons.
Every hadron has an antiparticle, built from the corresponding antiquarks. An antibaryon is three antiquarks (q̅q̅q̅).
Note that the antineutron is not the same as the neutron, even though both are uncharged: their baryon numbers are −1 and +1, so they are genuinely different particles.
Because a meson already contains an antiquark, the antiparticle of a meson is another meson. Replacing every quark by its antiquark turns π⁺ (ud̅) into π⁻ (u̅d), so the two charged pions are antiparticles of each other. The same is true of K⁺ and K⁻. The π⁰ is its own antiparticle.