nuclear fission
the splitting of a heavy nucleus into lighter nuclei. releases energy
nuclear fission - chain reaction
nucleus is struck by neutron - splits into nuclei and more neutrons are ejected, colliding with other nuclei and continuing fission, lasting until all material is used up
critical mass
a certain minimum mass of an element (uranium-235) that must be present, otherwise neutrons escape without causing further reaction
nuclear fusion
joining of two lighter nuclei to produce a heavier nucleus. energy is released due to mass defect
energy of nuclei undergoing fusion
kinetic energy of the nuclei has to be very high to overcome electrostatic repulsion
rutherford geiger marsden particle scattering experiment
alpha particles were directed at thin gold foil in vacuum chamber. the number of particles deflected at different angles were recorded
why does fusion occur at low values of A
because attractive nuclear forces between nucleons dominate over repulsive electrostatic forces between protons
why is energy released in fusion
the mass of nucleus created is slightly less than total combined mass of original nuclei. the mass defect is equal to binding energy released since the nucleus formed is more stable
why does fission occur at high values of A
repulsive electrostatic forces between protons begin to dominate, and these forces tend to break apart the nucelus
why is energy released in fission
an unstable nucleus is converted into stable nuclei with lower total mass - the mass defect is equal to binding energy released
fusion vs fission
fusion releases more energy per kg. the gradient of binding energy per nucleus much stepper at lower A values (when fusion occurs), meaning larger binding energy per nucleon is released
majority of alpha particles went through foil suggesting that:
the atom is mainly empty space
some alpha aprticles deflected at small angles suggesting:
there is a pos nucleus at the centre, repelling the positively charged alpha particle
a very small number of alpha particles deflected at large angles suggesting:
that the nucleus is extremely small and chrage of atom is concentrated
elementary/fundamental particle
particles not made up of any smaller components
quarks
fundamental particles that make up other subatomic particles, eg neutron and proton
hadrons
particle made up of quarks
flavours of quark
up u, charm c, top t, down d, strange s, bottom b
uct quark charge
+2/3
dsb quark charge
-1/3
anti particles
same mass but all properties are opposite, eg charge, baryon number, strangeness…
proton
uud
neutron
ddu
baryon
particle made of three quarks (no anti quarks)
meson
pair of quark and anti quark
baryon number for quarks
+1/3 (antiquarks have -1/3)
strangeness
strange quark has -1, anti strange has 1, everything else 0
when is strangeness not always conserved
weak interaction
conservation
charge, baryon number, lepton family number always, strangeness sometimes
leptons
fundamental particle, not made up of quarks
types of leptons
electron, muon, tau, electron neutrino, muon neutrino, tau neutrino
mass of leptons
tau heaviest, then muon, then electron. neutrinos have negligible amost zero mass
what force do leptons interact with
all weak nuclear force/interaction, those that have charge also with electromagnetic interaction
family lepton number
all leptons have lepton number of +1, just belongs to different families
what force do quarks interact with
strong, electromagnetic, weak
protons as baryons
the most stable baryon, has the longest half life and is lightest - cannot decay into lighter particle
beta minus decay
neutron turns into proton - the down quark turns into an up quark, antineutrino and electron also emmitted
beta plus decay
proton turns into neutron - up quark turns into down quark + positron + neutrino
pions
pos (u and anti d), neg (anti u and d) and neutral (u and anti u or d and anti d). lightest mesons, most stable. exchange particle of strong force
kaons
pos (u and anti s), neg (anti u and s) and neutral (anti d and s or d and anti s). heavy and unstable, decay into pions. long lifetimes (characteristic of particles w strange quarks). decay through weak interaction
strange particles
contain strange quark. produced through strong interaction, decay through weak
strong nuclear force
holds the nucleus together against electromagnetic repulsion. very short range. keeps quarks bound within nucleus
range of strong force
repulsive until 0.5fm
attractive from 0.5 to 3fm
max attractiveness at 1fm
zero after 3fm
exchange particles of strong interaction
pion (between nucleons) and gluon (between quarks) - hadrons subject to interaction since made up of quarks
leptons and strong force
leptons cannot interact w strong force since not made of quarks
weak nuclear force
responsible for radioactive decay of atoms
exchange particles of weak force
w-, w+, z0 bosons - depends on type of interaction
boson used in beta minus decay
w- boson
exchange particle used in beta plus decay
w+ boson
exchange particles of strong force
gluons and mesons
exchange particle of electromagnetic interaction
photon
gravitational exchange particle
graviton
quark confinement
it is impossible to have isolated quarks - they have never been found on their own, only in mesons or baryons
higgs boson
a particle responsible through its interactions for the mass od the particles od the standard model, in particular for masses of w and z bosons
electron capture
an electron is absorbed by a proton in the nucleus, resulting in release of a neutron and electron neutrino - mediated by w+ boson
electron proton collision
an electron collides with a proton, and a neutron and electron neutrino is emmitted - mediated by w- boson
properties of photon
no mass, no charge, its own antiparticle
exchange particles
virtual particles/bosons that mediate/carry/transmit the fundamental force between interacting particles - when two particles exert a force on each other, a virtual particle is created
graviton
only theoretical, no mass, no charge, its own anti particle