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Physics (AS & A Level) 9702 · Chapter 11

Particle physics

The alpha-scattering experiment, the nuclear atom, nuclide notation and isotopes, alpha, beta and gamma radiation, antiparticles and neutrinos, decay equations, quarks, hadrons and leptons.

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11.1 Atoms, nuclei and radiation

Alpha-particle scattering

Alpha particles were fired at a very thin gold foil in a vacuum.

ObservationWhat it shows
Most went straight throughthe atom is mostly empty space
A few were deflected through small anglesthere is a concentrated positive charge
A very few (about 1 in 8000) bounced back through more than 90°that charge and nearly all the mass are in a very small nucleus

Alpha particles passing a gold nucleus: most go straight on, one is deflected a little, and one close to the nucleus turns back

Alpha particles passing a gold nucleus: most go straight on, one is deflected a little, and one close to the nucleus turns back

Nuclei have diameters of about 10−1510^{-15} m, while atoms are about 10−1010^{-10} m across.

The nuclear atom and nuclides

The nucleus contains protons and neutrons (together called nucleons), and electrons orbit it. A nuclide is written ZAX^{A}_{Z}\text{X}:

  • AA is the nucleon number, which is protons plus neutrons.
  • ZZ is the proton number.

Isotopes are forms of the same element, with the same number of protons but different numbers of neutrons. For example, 92235U^{235}_{92}\text{U} and 92238U^{238}_{92}\text{U}.

The unified atomic mass unit is 1 u=1.66×10−271\ \text{u} = 1.66 \times 10^{-27} kg, about the mass of one nucleon.

Radiation

RadiationCompositionMassCharge
α\alphahelium nucleus, two protons and two neutrons4 u+2e+2e
β−\beta^-electronabout 11800\tfrac{1}{1800} u−e-e
β+\beta^+positronabout 11800\tfrac{1}{1800} u+e+e
γ\gammaelectromagnetic radiation00

Antiparticles and neutrinos

An antiparticle has the same mass as its particle but the opposite charge. The positron is the antiparticle of the electron.

  • β−\beta^- decay also emits an electron antineutrino, νˉ\bar{\nu}.
  • β+\beta^+ decay also emits an electron neutrino, ν\nu.

Alpha particles from a given decay have discrete energies. Beta particles have a continuous range of energies, because the energy released is shared between the beta particle and the (anti)neutrino in varying proportions.

Decay equations

Nucleon number and charge are conserved in nuclear processes.

92238U→ 90234Th+24α^{238}_{92}\text{U} \rightarrow\, ^{234}_{90}\text{Th} + ^{4}_{2}\alpha

614C→ 714N+−10β+νˉ^{14}_{6}\text{C} \rightarrow\, ^{14}_{7}\text{N} + ^{0}_{-1}\beta + \bar{\nu}

611C→ 511B++10β+ν^{11}_{6}\text{C} \rightarrow\, ^{11}_{5}\text{B} + ^{0}_{+1}\beta + \nu

11.2 Fundamental particles

Quarks

A quark is a fundamental particle. There are six flavours. Each has an antiquark with the opposite charge.

QuarkChargeAntiquark charge
up (u), charm (c), top (t)+23e+\tfrac{2}{3}e−23e-\tfrac{2}{3}e
down (d), strange (s), bottom (b)−13e-\tfrac{1}{3}e+13e+\tfrac{1}{3}e

Hadrons

Protons and neutrons are not fundamental. They are made of quarks.

  • A hadron is any particle made of quarks.
  • A baryon has three quarks. Proton = uud (charge +23+23−13=+1+\tfrac{2}{3} + \tfrac{2}{3} - \tfrac{1}{3} = +1). Neutron = udd (charge +23−13−13=0+\tfrac{2}{3} - \tfrac{1}{3} - \tfrac{1}{3} = 0).
  • A meson has one quark and one antiquark.

Quark changes in beta decay

β−:d→u+e−+νˉ(a neutron becomes a proton)\beta^-: \quad \text{d} \rightarrow \text{u} + e^- + \bar{\nu} \qquad (\text{a neutron becomes a proton})

β+:u→d+e++ν(a proton becomes a neutron)\beta^+: \quad \text{u} \rightarrow \text{d} + e^+ + \nu \qquad (\text{a proton becomes a neutron})

Leptons

Electrons and neutrinos are fundamental particles called leptons. They are not made of quarks, and they do not count as hadrons.

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