the strong nuclear force is attractive up to approximately 3 fm
the strong nuclear force is repulsive closer than approximately 0.5 fm
some atomic nuclei are unstable. the nucleus gives out radiation as it changes to become more stable. this is a random process called radioactive decay
an alpha particle consists of two neutrons and two protons
an alpha particle is the same as a helium nucleus
a beta particle (β-) is a high speed electron ejected from the nucleus
during beta-minus (β-) decay a neutron turns into a proton, emitting a beta-minus particle and an electron antineutrino in the process
the existence of the neutrino was hypothesised to account for conservation of energy in beta decay
for every type of particle there is a correspondingantiparticle
the antiparticle of the proton is the antiproton
the antiparticle of the neutron is the antineutron
the antiparticle of the electron is the positron
the antiparticle of the neutrino is the antineutrino
a particle and its antiparticle have identical masses
a particle and its antiparticle have opposite charge that are equal in magnitude
a particle and its antiparticle have identical rest energies
a photon is a packet or 'quantum' of electromagnetic waves
the energy of a photon is directly proportional to its frequency
E=hf
the energy of a photon is inversely proportional to its wavelength
E=hc/λ
annihilation occurs when a particle and its corresponding antiparticle meet and their mass is converted into radiation energy in the form of two photons
two photons are released (travelling in opposite directions) as a result of annihilation in order to conserve both momentum and energy
following annihilation the minimum total energy of the two photons produced is equal to the total rest energy of the particle-antiparticle pair
in pair production a photon creates a particle and its corresponding antiparticle providing that the photon has enough energy to produce their rest masses
in order for pair production to occur the photon must have energy greater than the total rest energy of the particle-antiparticle pair produced. any excess energy is transferred to the kinetic energy store of the particles
hadrons are subject to the strong force
there are two classes of hadrons: baryons and mesons
the proton is an example of a baryon
uud
the neutron is an example of a baryon
udd
the pion is an example of a meson
π- = du ¯
π+ = uu ¯, dd ¯
π0 = ud ¯
the kaon is an example of a meson
K- = su ¯
K+ = us ¯
K0 = ds ¯, sd ¯
baryon number must be conserved in all interactions
the proton is the only stable baryon into which other baryons eventually decay into
the pion is the exchange particle of the strong nuclear force