Theme E — Nuclear and Quantum Physics
E.3.5 Activity and Half-Life — IB Physics HL Revision Notes & Topical Questions
5 min read 8 parts Lesson 22 of 45 1 quiz
Curriculum Equation Key Radioactive Decay & Half-Life FormulasFast Exam Solution
N(t) = N₀ × (1/2)t / t½ | λ = ln(2) / t½ ≈ 0.693 / t½ | E = Δm × c²
Lesson summary
E.3.5 Activity and Half-Life — IB PHYSICS SL notes: Define activity and half-life and use them to predict how a radioactive sample decays.Activity = the number of nuclei in a sample that decay per unit time.Its SI unit is the becquerel (Bq), where 1 Bq is one decay per second.Act…
- Activity and count rate
- It is a constant for a given isotope
- It is impossible to predict when one nucleus decays
- The same fall is seen at every stage
- After two half-lives one quarter remains
- Fraction decayed
Part 1 of 5Half-life
1Half-life
Half-life the time taken for half of the undecayed nuclei of a nuclide to decay, or for the activity of the source to fall to half.
- The time for the corrected count rate to halve is also the half-life.
2It is a constant for a given isotope
- It is a constant for a given isotope it does not depend on the number of nuclei, temperature or chemical state.
3It is impossible to predict when one nucleus decays
- It is impossible to predict when one nucleus decays but the behaviour of a large sample can be predicted from its half-life.
4
Half-lives range from a fraction of a second to billions of years.
- Technetium-99m is about 6 hours and iodine-131 about 8 days.
- Carbon-14 is about 5700 years and uranium-235 about 704 million years.
- Uranium-238 is about 4.5 billion years.
Part 2 of 5Pattern of decay over half-lives
1
Each half-life halves the number of undecayed nuclei and the activity.
- After n half-lives the proportion remaining = (1/2)n.
- The number of half-lives is n = elapsed time divided by the half-life.
2The same fall is seen at every stage
- The same fall is seen at every stage the time to go from 100% to 50% equals the time to go from 50% to 25%.
| Half-lives passed | Proportion remaining | Activity |
|---|---|---|
| 0 | 1 | A0 |
| 1 | 1/2 | A0/2 |
| 2 | 1/4 | A0/4 |
| 3 | 1/8 | A0/8 |
| 4 | 1/16 | A0/16 |
1After two half-lives one quarter remains
- After two half-lives one quarter remains not zero.
2Fraction decayed
1 minus the fraction remaining — so after 5 half-lives 31/32 has decayed.
Part 3 of 5Decay curves and measuring half-life
1
Measure the initial activity A0 of the sample.
2
Measure how the activity (or corrected count rate) changes with time.
3
Subtract the background count rate from every reading.
4
Plot corrected count rate against time and draw a smooth best-fit curve.
5
Read the time for the value to fall to half; repeat from several starting values and take the mean.
Decay curves and measuring half-life
The curve is exponential
- The curve is exponential it becomes less steep but never reaches zero.
If background is not subtracted, the curve levels off at a non-zero value and the half-life is wrong.
Real data scatter about the curve
- Real data scatter about the curve because decay is random.
Part 4 of 5Why half-life matters in practice
Why half-life matters in practice
Half-life decides how long a source stays useful or hazardous.
- A medical tracer needs a half-life of hours so that it is gone from the body quickly.
- Waste with a half-life of thousands of years needs very long storage.
For equal numbers of nuclei, the shorter half-life gives the larger activity
- For equal numbers of nuclei, the shorter half-life gives the larger activity but the source decays away sooner.
The number of undecayed nuclei halves every half-life
- The number of undecayed nuclei halves every half-life but the mass of the sample does not, because the stable daughter nuclei remain.
Part 5 of 5More from the specification
More from the specification
Decay constant and mechanical centripetal force
- Decay constant and mechanical centripetal force unstable radioisotopes decay exponentially over time, providing a radiometric means independent of external force.
Radioactive Activity and Half-Life
- The activity of a radioisotope decreases exponentially over time according to A = A0 * e^(-lambda * t), halving with each half-life interval t1/2 = ln(2) / lambda.
Alpha, Beta, and Gamma Radiation
- Unstable parent nuclei decay by emitting alpha particles, beta particles (electrons or positrons),
- (2 protons and 2 neutrons)
- or de-exciting via high-energy gamma rays.
Nuclear Binding Energy and Mass Defect
- The difference between the mass of an intact nucleus and the combined mass of its constituent protons and neutrons converts to binding energy via Einstein's relation Delta E = Delta m * c2.
Nuclear Stability and Particle Balance
- The ratio of neutrons to protons determines radioactive decay modes,
- as unstable nuclides emit radiation to achieve a more favorable binding energy per nucleon.
Ionising radiation
- Radiation with enough energy to remove electrons from atoms
Penetrating power
- How far radiation travels through a material.
Nuclear notation
- Symbol showing mass number and atomic number.
Beta-plus decay
- Proton changes to a neutron with emission of a positron and a neutrino.
Decay equation
- An equation in nuclide notation with balanced nucleon and proton numbers.
Radiation
- Transfer by electromagnetic waves, requiring no medium
Proton
- Positive particle in the nucleus, relative charge +1 and relative mass 1.
Neutron
- Neutral particle in the nucleus, relative mass 1.
Electron
- Negatively charged particle in an atom.
Binding energy
- The minimum energy required to separate the nucleons of a nucleus to infinity.
Background radiation
- Radiation that is always present in the environment.
Alpha particle
- Helium nucleus, charge +2.
Alpha decay
- Loss of 2 protons and 2 neutrons.
Key terms
| Term | Meaning |
|---|---|
| Activity | Number of nuclei decaying per unit time; unit becquerel (Bq). |
| Becquerel (Bq) | One decay per second. |
| Half-life | Time for half the undecayed nuclei, or the activity, to fall by half. |
| Exponential decay | Decay in which the rate is proportional to the amount present. |
| Count rate | Rate of pulses registered by a detector, a fraction of the activity. |
| Corrected count rate | Count rate with the background count rate subtracted. |
Avoid these mistakes
1
Believing all nuclei have decayed after two half-lives — one quarter remains.
2
Reading half-life from a graph not corrected for background — subtract background first.
3
Thinking half-life depends on the starting amount or temperature — it is constant for an isotope.
4
Confusing activity (decays per second) with count rate (detected counts) — the detector sees only a fraction.
5
Using the mass of the whole sample to track decay — only the undecayed radioactive nuclei halve.
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