Nuclear Physics Flashcards
Describe the experimental setup of the Rutherford scattering experiment.
Collimated beam of alpha particles.
Fire at a thin metal (gold) foil.
Fluorescent screen surrounding the whole apparatus
State the three observations of the scattering experiment.
Most alpha particles passed straight through.
Some alpha particles deflected by small angles.
Tiny number of alpha particles deflected by large angles (> 90 degrees)
State the three conclusions made from these observations of the scattering experiment.
The atom is mostly empty space (Nuclear radius «_space;atomic radius).
Nucleus must be positively charged to repel positive alpha particles.
Nearly all of atom’s mass concentrated in a very tiny nucleus.
What fundamental force is responsible for alpha particle scattering?
ElectroMAGNETIC force
What are the two methods used for determining the nuclear radius?
Distance of closest approach of alpha particles.
Electron scattering patterns.
Describe the energy changes of an alpha particle backscattering (180 degree deflection)
Alpha particle initially has kinetic energy.
As positive alpha particle approaches positive nucleus, kinetic energy is transferred into a store of electrical potential energy.
Why is the distance of closest approach only an estimate for the maximum nuclear radius?
Alpha particle never actually reaches the nucleus, only travels very close to it
Therefore, nuclear radius must be lower than closest approach distance.
Describe the experimental setup of electron scattering.
Collimated beam of electrons accelerated to relativistic speeds (energies of MeV).
Fired towards nuclei of thin film of material, onto a screen behind.
What is the adapted de Broglie wavelength equation for these high energy electrons?
λ ≃ hc / E
Describe the intensity-scattering angle interference pattern produced by electron scattering.
Bright central maximum.
Decreasing intensity as scattering angle increases.
Non-zero minima.
State the advantages of using the distance of closest approach for determining nuclear radius.
Uses simple calculations for a good estimate of maximum nuclear radius.
Only requires alpha particles to be accelerated to low speeds, compared to acceleration for relativistic electrons.
State the advantages of using the electron scattering method for determining nuclear radius.
Much more accurate value for nuclear radius, measured directly.
Electrons have a very small mass, so no recoil on nucleus compared to relatively larger alpha particles.
Derive the general expression for nuclear density. What does it show?
Mass of nucleus = A x mnucleon
V = 4/3 πR3 = 4/3 π (R0A1/3)3 = 4/3 πR03A
Density = mass / volume = 3mnucleon / 4πR03
Nuclear density is independent of mass number.
List the assumptions made when deriving the nuclear density.
Assumed protons have the same mass as neutrons – (protons have slightly lower mass).
Assumed nucleus is a perfect sphere – (shape is not perfectly spherical).
Density within a nucleus is uniform – (density is non-uniform).
Which nuclear instability causes radioactive decay of alpha, beta-minus, beta-plus and gamma?
Alpha – Heavy nuclei
Beta-minus – Too many neutrons (neutron-rich)
Beta-plus – Too many protons (proton-rich)
Gamma – Too much energy (highly energetic)
Describe the ionising effect, range in air, penetrating power and behaviour in magnetic/electric fields for alpha radiation.
Strongly ionising
Travels several cm in air
Stopped by paper or skin
Positive charge and relatively high mass, deflected by a small amount in fields
Describe the ionising effect, range in air, penetrating power and behaviour in magnetic/electric fields for beta radiation.
Weakly ionising
Travels a few m in air
Stopped by few mm of metal
Negative charge and relatively low mass, deflected by a large amount.
Describe the ionising effect, range in air, penetrating power and behaviour in magnetic/electric fields for gamma radiation.
Very weakly ionising
Travels tens to hundreds of m in air
Stopped by few cm of concrete or lead
No charge, so unaffected by fields.
Define the term background radiation and list 3 possible sources.
Radioactivity/nuclear radiation that is always present and cannot be eliminated.
Radon gas in the air.
Radioactive isotopes in rocks/ground/buildings.
Cosmic rays.
Medical application/waste.
Describe the process of calculating a corrected count rate.
Take multiple (at least three) readings of background radiation.
Average these readings, and subtract the average from the measured count rate from a radioactive source.
Describe the inverse-square law for gamma radiation.
Gamma radiation emitted in all directions.
Radiation spreads out as distance increases.
Less radiation per unit area = lower intensity of radiation.
Intensity decreases by the square of the distance from the source.
Describe the activity of a sample and give the unit. What is activity proportional to?
- The number of nuclei that decay per second - (Becquerels, Bq) - Activity is directly proportional to the number of nuclei in the sample (N)
What is the probability of a nucleus decaying per second called and why is a probability needed?
Probability of a given nucleus decay per second is called the decay constant (λ).
Probability is required as the decay of an individual nucleus is completely random – it cannot be exactly predicted.
Define the half-life of an isotope.
The average time it takes for the number of unstable nuclei to halve.
The longer the half-life, the longer an isotope stays radioactive.
T1/2 = ln2 / λ