Objective: Know that ionising nuclear radiation can be measured using a detector connected to a counter.
Think of a detector as a security guard who rings a bell every time a radioactive particle passes by. The guard (detector) is connected to a counter that keeps a tally of how many times the bell rings. The more particles that pass, the higher the count rate.
The activity of a radioactive source, measured in becquerels (Bq), is defined as the number of decays per second:
Activity: \$A = \frac{N}{t} \quad \text{with } 1\,\mathrm{Bq}=1\,\text{decay/s}\$
The counter records a count rate \$R\$, which is related to the activity by the detector efficiency \$\epsilon\$:
\$R = \epsilon A\$
| Detector | Principle | Typical Use | Example |
|---|---|---|---|
| Geiger–Müller Tube | Ionisation of gas → spark → pulse | General radiation checks | Geiger counter |
| Scintillation Detector | Particle excites crystal → light flash → photomultiplier | Medical imaging, high‑energy physics | NaI(Tl) detector |
| Semiconductor Detector | Charge carriers generated in a solid → current pulse | High‑resolution spectroscopy | Si(Li) detector |
The count rate \$R\$ (counts per minute) is proportional to the source activity, but the proportionality constant (efficiency) depends on the detector geometry and the type of radiation.
A detector is like a smart phone that records every “call” (decay) it receives. The counter is the phone’s dialer that keeps a running total. By understanding the detector’s efficiency, we can translate the raw counts into the true activity of the radioactive source.