Background radiation and half-life
Key idea: Atomic structure, nuclide notation, random decay, radiation properties, background radiation, half-life, applications and hazards.
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The core idea
Syllabus and review details
- K326 / K327 Science Physics componentK326 / K327 · 2027Checked against the syllabus · partial topic coverageRadioactivity topic 16(a)–(h), PDF pages 23–24
Separate the source from its surroundings
A detector records radiation from the source and background radiation from the environment. Background sources include cosmic rays, rocks and building materials, and naturally occurring radioactive substances in living things.
Those are natural sources. Artificial sources, such as operating medical X-ray equipment, can also contribute to radiation detected in the surroundings.
To compare readings fairly, use the same detector position and settings. Convert counts to count-rate before subtracting readings taken over different durations:
count-rate = counts/(counting time).
For example, a background observation of 100 counts in 5 minutes gives 20 counts/min. A source-present observation of 260 counts in 1 minute gives 260 counts/min. The estimated source contribution is 260-20 = 240 counts/min, not 260-100.
Counts fluctuate because nuclear decay is random. A longer background observation or repeated observations improve the estimate. Keep the source–detector arrangement unchanged while comparing decay readings; otherwise a falling reading could result from a change in distance.
What half-life describes
The half-life of a radioactive nuclide is the time for the number of undecayed nuclei, or its activity, to fall to half its initial value. With unchanged detecting conditions, the background-corrected source count-rate follows the same trend.
Each half-life leaves the same fraction, not the same number. After three half-lives, the expected remaining fraction is 1/2 × 1/2 × 1/2 = 1/8. This describes a large sample on average; it does not give an expiry time for any individual nucleus.
A larger sample of the same nuclide starts with a greater activity but has the same half-life. Detector count-rate is not automatically the source’s activity in becquerels: a detector does not register every decay.
Modelled example 1
Background correction before halving
Problem
A detector reads 460 counts/min beside a source. Background is 60 counts/min. After one half-life, what measured count-rate is expected on average?
Study the worked solution
Isolate the source
Method
Subtract the background reading.Reason
Only the source contribution halves.Working
Net count-rate = 460-60 = 400 counts/min.
Apply one half-life
Method
Halve the net source count-rate.Reason
After one half-life, the source activity is half its initial value.
Working
400/2 = 200 counts/min.Restore the measured background
Method
Add the unchanged background contribution.Reason
The detector continues to record environmental radiation.
Working
Measured count-rate = 200 + 60 = 260 counts/min.
Guided practice 2
Build a repeated-halving chain
Problem
A sample has a net count-rate of 640 counts/min and a half-life of 3 hours. Find its net count-rate after 9 hours.
Try this before viewing the solution
Hints
Hint 1: count intervals
Use n = t/T_(1/2).
Hint 2: show the chain
Write every halving rather than subtracting a fixed amount.
View solution step by step
Count half-lives
Method
Divide total time by one half-life.Reason
Each complete interval causes one halving.Working
n = 9/3 = 3.Halve three times
Method
Construct the sequence.Reason
Radioactive decay is exponential, not a constant subtraction.
Working
640 → 320 → 160 → 80 counts/min.
Infer half-life from raw observations
These are illustrative readings, not a real-source practical. Each source-present count was collected for one minute at the indicated elapsed time, using unchanged detector geometry. The independent background estimate is 20 counts/min. The points include small fluctuations; connecting segments only guide the eye.
Find half-life after subtracting background
Raw detector count-rates at 0, 5, 10 and 15 minutes, with a separate background estimate. Use the accessible data table to calculate the source contribution.
Scroll across the graph to read all labels.
View figure data
| Series | Time (min) | Time uncertainty | Count-rate (counts/min) | Count-rate uncertainty |
|---|---|---|---|---|
| Measured | 0 | 260 | ||
| Measured | 5 | 142 | ||
| Measured | 10 | 79 | ||
| Measured | 15 | 51 | ||
| Background | 0 | 20 | ||
| Background | 15 | 20 |
Guided practice 3
Find a halving interval
Problem
Use the observations in the plot or its data table. Find the corrected rates at 0 and 5 minutes, then estimate the half-life using these and the later readings.
Try this before viewing the solution
Hints
Hint 1: source contribution
Subtract the same background rate from every observation.
Hint 2: fractional change
Compare each corrected rate with half the preceding corrected rate. Small fluctuations need not give exact halves.
View solution step by step
Correct every observation
Method
Subtract 20 counts/min from each raw rate.Reason
Background does not decay with this source.Working
The corrected rates are 240, 122, 59 and 31 counts/min.
Compare fractional changes
Method
Look for approximately equal time intervals for halving.
Reason
Random readings need not halve exactly.Working
240 → about 120 → about 60 → about 30 at five-minute intervals gives an estimated half-life of about 5 min.
Apply the method independently
A second illustrative record uses one-minute counts at fixed geometry. Background is 30 counts/min.
| Elapsed time / min | Raw count-rate / counts/min |
|---|---|
| 0 | 350 |
| 4 | 190 |
| 8 | 110 |
| 12 | 70 |
Repair a first error
A learner writes: “The raw count-rate starts at 350, so after one half-life it is 175. I then subtract background.” Identify the first incorrect operation and find the expected raw reading after one half-life.
Practice and next step
Use the Radioactivity topic check for focused practice and feedback. Then continue to Applications, hazards and protection.
Continue with the next resource in this course.
Course and syllabus information
- Course
- SEC G3 Combined Science Physics component
- Edition
- SEC G3 Combined Science Physics component 2027