HALFLIFE
CHAMBER · 384 NUCLEI — s⁻¹ t½ = 16.0 s · compressed
Live · specimen 137-A

HALFLIFEWatch an unstable sample decay in real time — random up close, exact in the long run.

Fraction remaining
%
Elapsed
Population
Decays logged
Activity
s⁻¹
Fitted half-life · least squares
s
theoretical 16.0 s — the fit converges as decays accumulate
01 — What you're watching

No atom knows when it's its turn.

Every glowing point is one unstable nucleus. In any given second it has a fixed, tiny chance of decaying — and no memory of how long it has already waited.

That is the strange honesty of radioactive decay. A nucleus that has survived ten half-lives is no more likely to go in the next instant than a freshly made one. There is no ageing, no wear, no schedule. The flash you just saw was not due; it was rolled.

So the chamber flickers unpredictably. You cannot say which point will darken next, or exactly when. Watch one dot and it looks like pure chaos — a coin that keeps its own counsel.

02 — The law from the noise

Chaos, added up, is a clock.

Stop watching one atom and watch the crowd. The randomness cancels, and a clean exponential falls out — the curve drawing itself beside the panel.

Halve the sample, then halve what remains, then halve that. The time each halving takes is the same: one half-life. The panel fits a straight line to the decaying population and reads the half-life straight back out of the noise — 16 seconds, here, compressed from something that in nature might be minutes or four billion years.

Early on the fit wanders; a handful of events is not much of a crowd. Give it a few hundred decays and the fitted number settles onto the truth. That convergence — noise becoming law before your eyes — is the whole point of this instrument.

Left running, the sample empties, reseeds, and begins again.

03 — A range the eye can't hold

Half-lives from a heartbeat to the age of the Earth.

The same law spans sixty orders of magnitude. Every isotope below obeys exactly what the chamber shows — only the clock speed changes.

Polonium-214 α164 µsa flicker in a decay chain
Iodine-131 β⁻8.02 daysthyroid medicine, fallout
Cobalt-60 β⁻,γ5.27 yearssterilisation, radiotherapy
Caesium-137 β⁻30.17 yearsthe long shadow of a meltdown
Carbon-14 β⁻5,730 yearsdating bone, cloth, charcoal
Uranium-238 α4.468 Byrolder than the ground it sits in
µs → Byr · sixteen orders of magnitude, one identical law
04 — Reading the instrument
A · CHAMBER

The flash

Each decay lights a ring and, if you enable it, a Geiger tick. Bright cyan for the common event; a rarer amber flash marks a higher-energy decay — roughly one in forty.

B · CURVE

The trace

Cyan is the theoretical exponential. The scattered points are the sample's actual count, ticking along beside it. The amber line is the live fit — you watch it lock on.

C · LAST

The survivor

When only a few nuclei are left, the final one is ringed and labelled. Which atom outlasts all the others is decided by nothing but chance — and you can never call it early.