Ions produced by radiation carry a current
Practical Activity for 14-16
A radioactive source produces radiation that will ionise the air. The conducting air completes a circuit to charge an electroscope. Use the circuit to show the ionising effect of the radiation and present it as a means of detecting ionising radiation.
Apparatus and Materials
- Power supply, EHT, 0–5 kV (with internal safety resistor)
- Metal plates with insulating handles, 2
- Hook for electroscope
- Retort stands and bosses, 2
- Connecting leads
- Holder for radioactive source (e.g. forceps)
Health & Safety and Technical Notes
See guidance note on
A school EHT supply is limited to a maximum current of 5 mA. which is regarded as safe. For use with a spark counter, the 50 MΩ. safety resistor can be left in circuit so reducing the maximum shock current to less than 0.1 mA. Although the school EHT supply is safe, shocks can make the demonstrator jump. It is therefore wise to see that there are no bare high voltage conductors; use female 4 mm connectors where required.
A web cam or ‘flexicam’ could be used to project an image of the electroscope's gold leaf onto a screen. Alternatively, use a bright lamp to cast a shadow of the leaf on a screen or wall.
The advantage of using an EHT is that it looks like an electric circuit – albeit a strange one. The electroscope plays the part of very sensitive meter and the air between the plates is a component whose resistance changes.
Take care when using the electroscope not to make it all seem like a sleight of hand – especially when moving leads around.
Radium is a source of alpha, beta and gamma radiation however the beta and gamma radiation do not cause enough ionisation of the air to start a spark.
- Fix the two metal plates so that they are parallel to one another and about 1 cm apart.
- Connect one of the plates to the positive terminal of the E.H.T. supply through the safety resistor.
- Connect the other plate to the leaf of the electroscope through the hook.
- Connect the case of the electroscope to the negative terminal of the E.H.T. supply.
- Connect the negative terminal of the EHT supply to the earth terminal. Getting a current to flow and charge the electroscope
- Set the EHT supply to about 3 kV and switch it on. The leaf of the electroscope will rise due to induced charges; reset it by momentarily connecting the leaf to earth.
- Hold the sealed radium source beside the gap and point it between the plates; watch what happens. The air in the gap is ionised and allows a charge to flow across the gap; this charges the leaf of the electroscope.
- Discharge the electroscope by momentarily connecting the leaf to earth. Try recharging it by holding the source at different angles to and at different distances from the plates. Discharging the electroscope...
- You can also discharge the electroscope by ionising the air around it.
- Disconnect the electroscope from the supply but keep the base earthed. Replace the disc in the top of the electroscope and charge it using a flying lead from the positive terminal of the power supply (via the safety resistor).
- Point the sealed source over the top of the disc. This will ionise the air and allow the electroscope to discharge.
- Charge the electroscope again and try holding the sealed source at different angles and at different distances from the disc.
- The electroscope should discharge quickly to earth when the air above the its disc is ionised. If it is discharging too slowly, bring an earthed metal plate up close to the disc of the electroscope.
- In the demonstration
- As you bring the source towards the gap between the plates, point out that there is no flame and no obvious transfer of energy near the sealed source. Nevertheless, it must be producing ions in the gap. So it must be giving out some invisible radiation.
- Use the term “ionising radiation” to describe what the source is giving out.
- The circuit provides a visible means of detecting ionisation in the gap between the two plates. The electroscope provides the visibility and the high voltage across the air gap is the means of catching ions. This is the same principle as a more convenient detector (the Geiger-Müller tube) and it provides students with a conceptual step towards its construction. This is developed further in
This experiment was safety-tested in May 2007