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PhysicsA-Level 9 min read

Radioactive Decay & Half-Life

Drag along the decay curve and watch the count rate halve over each fixed half-life. Why decay is exponential — and what λ and half-life really mean.

The ScholarsGate Physics Team·Updated 08 Jul 2026

On this page

  • Decay is random but predictable
  • See it: the decay curve
  • Half-life and the decay constant
  • Worked example
  • Common mistakes
  • Practice
  • FAQ

You can never say whena single radioactive nucleus will decay — it might be in the next second or in a thousand years. Yet a lump of the same material fades away on a schedule so reliable we use it to date rocks and time medical scans. That tension between random and predictable is the whole story of half-life.

Random for one nucleus, precise for a trillion

Radioactive decay is spontaneous and random. Nothing you do — heating, squeezing, chemistry — changes when an individual nucleus will throw out its particle. Every undecayed nucleus has the same fixed probability of decaying in the next moment, and no memory of how long it has already waited.

The magic is in the numbers. A microgram of material holds billions upon billions of nuclei, and while you cannot predict any single one, the fractionthat decays each second is rock-steady. Randomness at the bottom becomes near-perfect regularity at the top — the same reason a casino always knows its monthly takings.

One nucleus is a coin you can’t time; a mole of them is a trillion coins flipped at once, and the average always lands where the maths says it will.

Read off the decay curve

Because a fixed fraction decays in each equal slice of time, the amount left follows a falling exponential. Pick the decay preset below and drag along the curve: over every fixed step the count rate drops to exactly half of what it was.

InteractiveThe decay curve
Loading interactive…
Choose the decay preset (e⁻ˣ) and drag along it — the count rate halves over each fixed half-life.
Text description ↓Hide text description ↑

An exponential curve for radioactive decay. Selecting the decay preset shows N falling towards zero; because decay is exponential, the quantity halves over each equal time interval — the constant half-life. Dragging along the curve reads off the remaining amount at a given time.

What the half-life measures

The half-life (t½) is the time taken for the quantity to fall to half its starting value. Its defining feature is that it is constant: whether you start with 8 grams or 8 milligrams, one half-life later exactly half remains, then half of that, and so on.

Half-life is tied to the decay constantλ — the probability per unit time that a given nucleus decays. The larger λ is, the faster the source drops and the shorter its half-life:

Linking λ and t½

λ = ln 2 / t½ ≈ 0.693 / t½. A big decay constant means a short half-life, and vice versa. The number of undecayed nuclei follows N = N₀e^(−λt), and the activity (decays per second, in becquerel) is A = λN — so the activity falls exponentially with exactly the same half-life as N.

Worked example

1Worked example — counting the halvings

A radioactive source has an activity of 800 Bq and a half-life of 6 hours. What is its activity after 18 hours?

18 hours is exactly three half-lives (18 ÷ 6 = 3). Each half-life halves the activity, so just follow the chain:

800 Bq → (6 h) → 400 Bq → (12 h) → 200 Bq → (18 h) → 100 Bq.

You could reach the same answer with A = A₀e^(−λt), using λ = ln 2 / 6 h ≈ 0.116 h⁻¹, but when the time is a whole number of half-lives, halving repeatedly is faster and less error-prone.

Common mistakes

Thinking half-life is half the time to fully decay

A half-life is not“halfway to empty”. After one half-life, half remains; after two, a quarter; after three, an eighth. The amount never quite reaches zero — each half-life only ever removes half of what is currently left.

Forgetting that the activity falls too

Both the number of undecayed nuclei andthe activity (the rate of decay) fall exponentially with the same half-life. If the count rate has dropped to a quarter, so has the number of nuclei — they are locked together by A = λN.

Practice

Your turn

A nuclide’s activity falls from 240 Bq to 30 Bq. How many half-lives have passed?

Show the answer ↓Hide the answer ↑

Halve until you reach 30: 240 → 120 → 60 → 30. That is three halvings, so three half-lives have passed.

Where it shows up

The same maths dates archaeological finds by carbon-14, sets the dose schedule for medical tracers, and governs how long nuclear waste stays hazardous — anywhere a quantity decays by a fixed fraction each step.

Key takeaways
  • Individual nuclear decay is spontaneous and random, but huge numbers of nuclei decay with precise, predictable statistics.
  • The half-life t½ is the constant time for the quantity — or the activity — to fall by half, whatever the starting amount.
  • The decay constant and half-life are linked by λ = ln 2 / t½.
  • The number of nuclei and the activity both decay exponentially: N = N₀e^(−λt) and A = λN.
  • To find the amount after a whole number of half-lives, just halve repeatedly.

Frequently asked questions

What is half-life?+
The half-life is the time taken for the number of undecayed nuclei (or the activity) to fall to half its value. Because decay is exponential, the half-life is constant: it takes the same time to go from 100% to 50% as from 50% to 25%.
Why is radioactive decay exponential?+
Each nucleus has a fixed probability of decaying per unit time, independent of the others, so the rate of decay is proportional to the number of nuclei present. A rate proportional to the amount always gives exponential decay: N = N₀e^{−λt}.
What is the decay constant?+
The decay constant λ is the probability per unit time that a given nucleus decays. It links to half-life by λ = ln 2 / t½, so a large λ means fast decay and a short half-life.
How are activity and the number of nuclei related?+
Activity A is the rate of decay, A = λN, so it is proportional to the number of undecayed nuclei. Since N decays exponentially, so does the activity — both fall by half each half-life.
SP

The ScholarsGate Physics Team

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