Introduction

Radioactivity is the spontaneous emission of radiations from unstable atomic nuclei. These radiations may be alpha particles, beta particles, gamma rays, or other nuclear emissions. Since radioactive radiations are invisible and can be harmful, they are detected using special instruments.

The choice of detector depends on the type of radiation, intensity, energy, dose rate, sensitivity required, and whether the aim is simple detection, dose measurement, or energy analysis.

Basic principle of radioactivity detection

Radioactive radiations interact with matter and produce measurable effects. Detection instruments convert these effects into visible tracks, electrical pulses, light flashes, darkening of film, or stored dose information.

Detection effect Used in
Ionization of gas GM counter, ionization chamber, proportional counter
Light emission Scintillation counter
Electron-hole pair formation Semiconductor detector
Condensation track Cloud chamber
Photographic darkening Film badge
Thermoluminescence TLD

Different methods of detecting radioactivity

  1. Geiger-Muller counter
  2. Ionization chamber
  3. Proportional counter
  4. Scintillation counter
  5. Semiconductor detector
  6. Cloud chamber
  7. Photographic film badge
  8. Thermoluminescent dosimeter

1. Geiger-Muller counter

Labelled diagram of Geiger-Muller counter showing mica window, gas-filled tube, anode wire, high voltage supply, ion avalanche and pulse counter
Neat labelled diagram of a Geiger-Muller counter.

The Geiger-Muller counter, or GM counter, is a gas-filled detector used for detecting alpha, beta and gamma radiations. It is one of the most popular radiation detectors because it is simple, portable and sensitive.

Theory

The GM counter works on the principle of ionization of gas followed by avalanche discharge. When radiation enters the GM tube, it ionizes the gas inside the tube. The electrons produced move towards the central anode wire and positive ions move towards the cathode wall.

A high potential difference is applied between anode and cathode. The electrons gain enough energy to produce further ionization. This produces an avalanche of ions and a large electrical pulse. Each pulse is counted as one radiation event.

Construction

Working

  1. Radiation enters the tube through the window or wall.
  2. The gas is ionized.
  3. Electrons accelerate towards the anode.
  4. Secondary ionization produces an avalanche.
  5. A large pulse is produced.
  6. The pulse is counted and may produce a click sound.

Procedure

  1. Connect the GM tube with the counter and high voltage supply.
  2. Switch on the instrument and allow it to stabilize.
  3. Record background count for one minute without source.
  4. Place the radioactive source at a fixed distance from the GM tube window.
  5. Record counts for a fixed time.
  6. Repeat readings and take the average.
  7. Subtract background count from observed count.

Observation and calculation

Corrected count rate = observed count rate – background count rate

Background count is due to cosmic rays and natural radioactivity, so background correction is necessary.

Plateau and dead time

The plateau region is the operating voltage range where count rate remains nearly constant with small voltage changes. The dead time is the short time after one count during which the tube cannot detect another event.

Advantages

Limitations

2. Ionization chamber

Labelled diagram of ionization chamber showing collecting electrodes, ion pairs in gas and electrometer
Neat labelled diagram of an ionization chamber.

Theory

An ionization chamber is a gas-filled detector operated at relatively low voltage. Radiation ionizes the gas, and the produced ions are collected by electrodes to give a small ionization current.

Procedure

  1. Connect the chamber to an electrometer.
  2. Apply suitable voltage.
  3. Expose the chamber to radiation.
  4. Measure the ionization current.
  5. Relate current to dose rate or radiation intensity.

Uses

Ionization chambers are useful for dose rate measurement, radiation therapy dosimetry, X-ray monitoring and gamma radiation measurement.

3. Proportional counter

Labelled diagram of proportional counter showing gas tube, anode wire, limited gas multiplication and pulse height analyzer
Neat labelled diagram of a proportional counter.

Theory

A proportional counter is operated at a voltage higher than an ionization chamber but lower than a GM counter. It produces gas multiplication, but the pulse height remains proportional to the energy deposited by the radiation.

Procedure

  1. Apply suitable proportional-region voltage.
  2. Allow radiation to enter the gas-filled tube.
  3. Collect pulses produced by limited gas multiplication.
  4. Analyze pulse height for energy information.

Uses

It is used for alpha and beta detection and where information about radiation energy is needed.

4. Scintillation counter

Labelled diagram of scintillation counter showing scintillator crystal, light flash, photomultiplier and counter
Neat labelled diagram of a scintillation counter.

Theory

In a scintillation counter, radiation strikes a scintillator and produces tiny flashes of light. These flashes are detected by a photomultiplier tube or photodiode and converted into electrical pulses.

Procedure

  1. Select a suitable scintillator such as NaI(Tl) for gamma rays.
  2. Place the radioactive source near the detector.
  3. Radiation produces light flashes in the scintillator.
  4. The photodetector converts light into electrical pulses.
  5. The pulses are counted or analyzed for energy.

Uses

Scintillation counters are used in gamma counting, nuclear medicine, environmental monitoring and radiation spectroscopy.

5. Semiconductor detector

Labelled diagram of semiconductor detector showing radiation entering crystal and electron-hole pair formation
Neat labelled diagram of a semiconductor detector.

Theory

Semiconductor detectors use materials such as silicon or germanium. Radiation creates electron-hole pairs in the semiconductor crystal. These charges are collected and converted into electrical signals.

Procedure

  1. Apply bias voltage to the semiconductor detector.
  2. Allow radiation to enter the active region.
  3. Electron-hole pairs are formed.
  4. Collected charges produce a signal.
  5. Signal processing gives count or energy spectrum.

Uses

Semiconductor detectors are used for high-resolution alpha, beta, X-ray and gamma spectroscopy.

6. Cloud chamber

Labelled diagram of cloud chamber showing supersaturated vapor, cold plate and condensation track
Neat labelled diagram of a cloud chamber.

Theory

A cloud chamber contains supersaturated vapor. Charged particles ionize the vapor, and droplets condense along the ionized path, making a visible track.

Procedure

  1. Create a supersaturated vapor region.
  2. Cool the base plate.
  3. Allow radiation to pass through the chamber.
  4. Observe visible tracks formed by condensation droplets.

Uses

Cloud chambers are useful for demonstration of alpha and beta particle tracks and for visual understanding of radiation paths.

7. Photographic film badge

Labelled diagram of photographic film badge showing film packet, filters and film darkening due to radiation
Neat labelled diagram of a photographic film badge.

Theory

A photographic film badge works because radiation darkens photographic film. The amount and pattern of darkening indicate radiation exposure.

Procedure

  1. Radiation worker wears the film badge during work.
  2. Radiation passes through filters and exposes the film.
  3. The film is later developed.
  4. Darkening is compared with standards to estimate dose.

Uses

Film badges are used for personal radiation monitoring in laboratories, hospitals and nuclear facilities.

8. Thermoluminescent dosimeter

Labelled diagram of thermoluminescent dosimeter showing TLD crystal, heating reader and light output
Neat labelled diagram of a thermoluminescent dosimeter.

Theory

A thermoluminescent dosimeter, or TLD, stores energy from radiation in a crystal. When the crystal is heated in a reader, it emits light. The emitted light is proportional to the radiation dose.

Procedure

  1. Wear or place the TLD in the radiation field.
  2. The crystal stores energy during exposure.
  3. After exposure, heat the TLD in a reader.
  4. Measure the emitted light.
  5. Calculate the absorbed dose.

Uses

TLDs are widely used for personal dose monitoring, medical dosimetry and environmental radiation measurement.

Comparison of radioactivity detection methods

Detector Main principle Best use Main limitation
GM counter Gas ionization and avalanche pulse Routine detection No accurate energy measurement
Ionization chamber Ionization current Dose rate measurement Less sensitive for weak radiation
Proportional counter Pulse proportional to deposited energy Particle detection with energy information Requires stable voltage operation
Scintillation counter Radiation produces light flashes Gamma counting and spectroscopy Needs optical detector
Semiconductor detector Electron-hole pair formation High-resolution spectroscopy Costly; may need cooling
Cloud chamber Condensation tracks Visual demonstration Not routine quantitative counting
Film badge Film darkening Personal monitoring No instant reading
TLD Light emission on heating Personal dose measurement Needs reader after exposure

Precautions while using radioactive sources

Summary

Most common detector Geiger-Muller counter
GM principle Gas ionization followed by avalanche discharge
GM output Electrical pulse/count
Important correction Background count correction
Important limitation Cannot measure energy accurately
Best energy resolution Semiconductor detector
Personal monitoring Film badge and TLD

References and further reading

  1. Glenn F. Knoll, Radiation Detection and Measurement.
  2. IAEA educational resources on radiation monitoring and radiation protection instruments.
  3. NCERT Chemistry, radioactivity and nuclear chemistry related sections.
  4. National radiation safety training materials on survey meters, dosimeters and contamination monitoring.

Conclusion

Radioactivity can be detected by several methods based on ionization, scintillation, semiconductor charge formation, visible tracks, photographic action and thermoluminescence. The Geiger-Muller counter is most important for routine detection because it is simple, portable and sensitive. However, for accurate energy measurement, scintillation and semiconductor detectors are more suitable.

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