OCR H556 chapter questions and answers
CH23 Nuclear and Particle Physics — Questions
5 min read 8 parts Lesson 1 of 2
Lesson summary
CH23 Nuclear and Particle Physics (Questions) — OCR A LEVEL PHYSICS A H556 notes: Describe the structure of the atom and nucleus, the types of radioactive decay and the laws of radioactive decay.Rutherford scattering — Most alpha particles pass through gold foil, a few are deflec…
- Nuclear notation
- Nuclear radius
- Strong nuclear force
- Electrostatic repulsion
- Alpha decay
- Beta-minus decay
Section 1 of 8Atomic structure and the nucleus
Atomic structure and the nucleus
Rutherford scattering
- Most alpha particles pass through gold foil, a few are deflected through large angles, showing a small, dense, positive nucleus.
Nuclear notation
- The nuclide is written with its proton number Z and nucleon number A, as A over Z X.
Isotopes
- Nuclei with the same number of protons but different numbers of neutrons.
Nuclear radius
- R = r0 A1/3 with r0 about 1.2 fm, so nuclear density is about the same for all nuclei.
Strong nuclear force
- It attracts nucleons at short range and becomes repulsive at very short distances below about 0.5 fm.
- (up to about 3 fm)
Electrostatic repulsion
- The nucleus is stable when the strong force outweighs the repulsion between protons.
Section 2 of 8Radioactive emissions
| Radiation | Nature | Ionising power | Penetration |
|---|---|---|---|
| Alpha | Helium nucleus (2 protons, 2 neutrons) | Strong | Stopped by paper or a few cm of air |
| Beta minus | Fast electron | Medium | Stopped by a few mm of aluminium |
| Gamma | High-energy photon | Weak | Reduced by thick lead or concrete |
Alpha decay
- The nucleus loses 4 nucleons and 2 protons: A decreases by 4 and Z by 2.
Beta-minus decay
- A neutron changes into a proton, releasing an electron and an antineutrino; Z increases by 1.
Beta-plus decay
- A proton changes into a neutron, releasing a positron and a neutrino; Z decreases by 1.
Conservation
- Nucleon number, charge and energy are conserved in each decay.
Antineutrino evidence
- Beta particles show a range of energies, so a third particle shares the energy.
Section 3 of 8Decay laws
Random and spontaneous
- Which nucleus decays next and when cannot be predicted.
Activity
- A = change in N / change in t, measured in becquerel.
- (decays per second)
Decay constant
- A = lambda N, where lambda is the probability of decay per unit time.
Exponential decay
- N = N0 e-lambda t and A = A0 e-lambda t.
Half-life
- The time for the number of undecayed nuclei or the activity to halve: t1/2 = ln 2 / lambda = 0.693 / lambda.
Example
- A source with half-life 6.0 hours has activity reduced to 1/8 after 18 hours.
Background radiation
- Radiation from rocks, cosmic rays and medical sources must be subtracted from count rates.
Section 4 of 8Using radioactivity
Radiocarbon dating
- The fraction of carbon-14 remaining in organic matter gives its age, using a half-life of 5730 years.
Thickness gauging
- Beta particles passing through a sheet are detected, and a falling count signals an increase in thickness.
Smoke detectors
- Alpha particles ionise air in the detector, and smoke reduces the current.
Safety
- Use tongs, keep time short, increase distance, and use shielding.
Detection
- A Geiger-Muller tube counts ionising radiation.
Section 5 of 8Detection and experiments
Detection and experiments
Absorption experiment
- Place different absorbers between a source and a detector and record the count rate.
Inverse square law for gamma
- The count rate falls with the square of the distance from a point source.
Cloud chamber
- Alpha particles leave thick, straight tracks, and beta particles leave thin, wandering tracks.
Half-life experiment
- Plot ln(count rate) against time; the gradient is -lambda.
Uranium series
- Radioactive decay series pass through many isotopes until a stable lead isotope is reached.
Hazards
- Ionising radiation damages DNA and can cause cancer.
Dose
- Exposure is reduced by limiting time, using shielding and keeping a distance.
Section 6 of 8Worked examples
A sample has an initial activity of 640 Bq and a half-life of 12 minutes. Calculate the activity after 48 minutes. [2]2 marks
Worked examples48 minutes is 4 half-lives.Activity = 640 / 16 = 40 Bq.Write the nuclear equation for the alpha decay of uranium-238 (Z = 92). [2]2 marks
Worked examples238U gives 234Th (Z = 90) plus an alpha particle 4He (Z = 2).Nucleon number: 238 = 234 + 4 and charge: 92 = 90 + 2.A radioactive isotope has a decay constant of 0.0231 s-1. Calculate its half-life. [2]2 marks
Worked examplest1/2 = ln 2 / lambda = 0.693 / 0.0231.t1/2 = 30 s.
Section 7 of 8Key terms
| Term | Meaning |
|---|---|
| Isotope | Atoms of the same element with different numbers of neutrons. |
| Half-life | The time for the activity to halve. |
| Decay constant | The probability of decay per unit time. |
| Activity | The number of decays per second. |
| Becquerel | One decay per second. |
| Nucleon | A proton or neutron. |
| Background radiation | Ionising radiation always present in the environment. |
| Strong nuclear force | The attractive short-range force between nucleons. |
Section 8 of 8Exam technique
1
Writing that radioactive decay is affected by temperature or chemical state.
2
Forgetting to subtract background radiation.
3
Mixing up the proton number and nucleon number in equations.
4
Saying alpha particles are the most penetrating.