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There are two types of detected radiation readout: counts or radiation dose. The counts display is the simplest and is the number of ionizing events detected displayed either as a count rate, such as "counts per minute" or "counts per second", or as a total number of counts over a set time period an integrated total.

The counts readout is normally used when alpha or beta particles are being detected. More complex to achieve is a display of radiation dose rate, displayed in a unit such as the sievert which is normally used for measuring gamma or X-ray dose rates.

A Geiger—Müller tube can detect the presence of radiation, but not its energy , which influences the radiation's ionizing effect.

Consequently, instruments measuring dose rate require the use of an energy compensated Geiger—Müller tube, so that the dose displayed relates to the counts detected.

The readout can be analog or digital, and modern instruments offer serial communications with a host computer or network. There is usually an option to produce audible clicks representing the number of ionization events detected.

This is the distinctive sound normally associated with handheld or portable Geiger counters. The purpose of this is to allow the user to concentrate on manipulation of the instrument whilst retaining auditory feedback on the radiation rate.

There are two main limitations of the Geiger counter. Because the output pulse from a Geiger—Müller tube is always of the same magnitude regardless of the energy of the incident radiation , the tube cannot differentiate between radiation types.

This is an insensitive period after each ionization of the gas during which any further incident radiation will not result in a count, and the indicated rate is, therefore, lower than actual.

Typically the dead time will reduce indicated count rates above about 10 4 to 10 5 counts per second depending on the characteristic of the tube being used.

The intended detection application of a Geiger counter dictates the tube design used. Consequently, there are a great many designs, but they can be generally categorized as "end-window", windowless "thin-walled", "thick-walled", and sometimes hybrids of these types.

The first historical uses of the Geiger principle were for the detection of alpha and beta particles, and the instrument is still used for this purpose today.

For alpha particles and low energy beta particles, the "end-window" type of a Geiger—Müller tube has to be used as these particles have a limited range and are easily stopped by a solid material.

Therefore, the tube requires a window which is thin enough to allow as many as possible of these particles through to the fill gas.

The window is usually made of mica with a density of about 1. The "pancake" Geiger—Müller tube is a variant of the end-window probe, but designed with a larger detection area to make checking quicker.

However, the pressure of the atmosphere against the low pressure of the fill gas limits the window size due to the limited strength of the window membrane.

Some beta particles can also be detected by a thin-walled "windowless" Geiger—Müller tube, which has no end-window, but allows high energy beta particles to pass through the tube walls.

Although the tube walls have a greater stopping power than a thin end-window, they still allow these more energetic particles to reach the fill gas.

End-window Geiger counters are still used as a general purpose, portable, radioactive contamination measurement and detection instrument, owing to their relatively low cost, robustness and their relatively high detection efficiency; particularly with high energy beta particles.

Geiger counters are widely used to detect gamma radiation and X-rays collectively known as photons , and for this the windowless tube is used.

However, detection efficiency is low compared to alpha and beta particles. The article on the Geiger—Müller tube carries a more detailed account of the techniques used to detect photon radiation.

These enter and ionize the fill gas. This is necessary as the low-pressure gas in the tube has little interaction with higher energy photons.

However, as photon energies decrease to low levels there is greater gas interaction and the direct gas interaction increases.

At very low energies less than 25 KeV direct gas ionisation dominates and a steel tube attenuates the incident photons. Consequently, at these energies, a typical tube design is a long tube with a thin wall which has a larger gas volume to give an increased chance direct interaction of a particle with the fill gas.

Above these low energy levels, there is a considerable variance in response to different photon energies of the same intensity, and a steel-walled tube employs what is known as "energy compensation" in the form of filter rings around the naked tube which attempts to compensate for these variations over a large energy range.

A variation of the Geiger tube is used to measure neutrons , where the gas used is boron trifluoride or helium-3 and a plastic moderator is used to slow the neutrons.

This creates an alpha particle inside the detector and thus neutrons can be counted. The term "Geiger counter" is commonly used to mean a hand-held survey type meter, however the Geiger principle is in wide use in installed "area gamma" alarms for personnel protection, and in process measurement and interlock applications.

A Geiger tube is still the sensing device, but the processing electronics will have a higher degree of sophistication and reliability than that used in a hand held survey meter.

For hand-held units there are two fundamental physical configurations: the "integral" unit with both detector and electronics in the same unit, and the "two-piece" design which has a separate detector probe and an electronics module connected by a short cable.

In the s a mica window was added to the cylindrical design allowing low-penetration radiation to pass through with ease.

The integral unit allows single-handed operation, so the operator can use the other hand for personal security in challenging monitoring positions, but the two piece design allows easier manipulation of the detector, and is commonly used for alpha and beta surface contamination monitoring where careful manipulation of the probe is required or the weight of the electronics module would make operation unwieldy.

A number of different sized detectors are available to suit particular situations, such as placing the probe in small apertures or confined spaces.

Gamma and X-Ray detectors generally use an "integral" design so the Geiger—Müller tube is conveniently within the electronics enclosure. This can easily be achieved because the casing usually has little attenuation, and is employed in ambient gamma measurements where distance from the source of radiation is not a significant factor.

However, to facilitate more localised measurements such as "surface dose", the position of the tube in the enclosure is sometimes indicated by targets on the enclosure so an accurate measurement can be made with the tube at the correct orientation and a known distance from the surface.

There is a particular type of gamma instrument known as a "hot spot" detector which has the detector tube on the end of a long pole or flexible conduit.

These are used to measure high radiation gamma locations whilst protecting the operator by means of distance shielding. Particle detection of alpha and beta can be used in both integral and two-piece designs.

In integral instruments using an end window tube there is a window in the body of the casing to prevent shielding of particles.

There are also hybrid instruments which have a separate probe for particle detection and a gamma detection tube within the electronics module.

The detectors are switchable by the operator, depending the radiation type that is being measured. In the United Kingdom the National Radiological Protection Board issued a user guidance note on selecting the best portable instrument type for the radiation measurement application concerned.

In Hans Geiger , under the supervision of Ernest Rutherford at the Victoria University of Manchester now the University of Manchester , developed an experimental technique for detecting alpha particles that would later be used to develop the Geiger—Müller tube in The fundamental ionization mechanism used was discovered by John Sealy Townsend between and , [7] and is known as the Townsend discharge , which is the ionization of molecules by ion impact.

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Although the tube walls have a greater stopping power than a thin end-window, they still allow these more energetic particles to reach the fill gas.

End-window Geiger counters are still used as a general purpose, portable, radioactive contamination measurement and detection instrument, owing to their relatively low cost, robustness and their relatively high detection efficiency; particularly with high energy beta particles.

Geiger counters are widely used to detect gamma radiation and X-rays collectively known as photons , and for this the windowless tube is used.

However, detection efficiency is low compared to alpha and beta particles. The article on the Geiger—Müller tube carries a more detailed account of the techniques used to detect photon radiation.

These enter and ionize the fill gas. This is necessary as the low-pressure gas in the tube has little interaction with higher energy photons.

However, as photon energies decrease to low levels there is greater gas interaction and the direct gas interaction increases.

At very low energies less than 25 KeV direct gas ionisation dominates and a steel tube attenuates the incident photons.

Consequently, at these energies, a typical tube design is a long tube with a thin wall which has a larger gas volume to give an increased chance direct interaction of a particle with the fill gas.

Above these low energy levels, there is a considerable variance in response to different photon energies of the same intensity, and a steel-walled tube employs what is known as "energy compensation" in the form of filter rings around the naked tube which attempts to compensate for these variations over a large energy range.

A variation of the Geiger tube is used to measure neutrons , where the gas used is boron trifluoride or helium-3 and a plastic moderator is used to slow the neutrons.

This creates an alpha particle inside the detector and thus neutrons can be counted. The term "Geiger counter" is commonly used to mean a hand-held survey type meter, however the Geiger principle is in wide use in installed "area gamma" alarms for personnel protection, and in process measurement and interlock applications.

A Geiger tube is still the sensing device, but the processing electronics will have a higher degree of sophistication and reliability than that used in a hand held survey meter.

For hand-held units there are two fundamental physical configurations: the "integral" unit with both detector and electronics in the same unit, and the "two-piece" design which has a separate detector probe and an electronics module connected by a short cable.

In the s a mica window was added to the cylindrical design allowing low-penetration radiation to pass through with ease. The integral unit allows single-handed operation, so the operator can use the other hand for personal security in challenging monitoring positions, but the two piece design allows easier manipulation of the detector, and is commonly used for alpha and beta surface contamination monitoring where careful manipulation of the probe is required or the weight of the electronics module would make operation unwieldy.

A number of different sized detectors are available to suit particular situations, such as placing the probe in small apertures or confined spaces.

Gamma and X-Ray detectors generally use an "integral" design so the Geiger—Müller tube is conveniently within the electronics enclosure. This can easily be achieved because the casing usually has little attenuation, and is employed in ambient gamma measurements where distance from the source of radiation is not a significant factor.

However, to facilitate more localised measurements such as "surface dose", the position of the tube in the enclosure is sometimes indicated by targets on the enclosure so an accurate measurement can be made with the tube at the correct orientation and a known distance from the surface.

There is a particular type of gamma instrument known as a "hot spot" detector which has the detector tube on the end of a long pole or flexible conduit.

These are used to measure high radiation gamma locations whilst protecting the operator by means of distance shielding. Particle detection of alpha and beta can be used in both integral and two-piece designs.

In integral instruments using an end window tube there is a window in the body of the casing to prevent shielding of particles.

There are also hybrid instruments which have a separate probe for particle detection and a gamma detection tube within the electronics module.

The detectors are switchable by the operator, depending the radiation type that is being measured. In the United Kingdom the National Radiological Protection Board issued a user guidance note on selecting the best portable instrument type for the radiation measurement application concerned.

In Hans Geiger , under the supervision of Ernest Rutherford at the Victoria University of Manchester now the University of Manchester , developed an experimental technique for detecting alpha particles that would later be used to develop the Geiger—Müller tube in The fundamental ionization mechanism used was discovered by John Sealy Townsend between and , [7] and is known as the Townsend discharge , which is the ionization of molecules by ion impact.

It was not until that Geiger and Walther Müller a PhD student of Geiger developed the sealed Geiger—Müller tube which used basic ionization principles previously used experimentally.

Small and rugged, not only could it detect alpha and beta radiation as prior models had done, but also gamma radiation. As the tube output required little electronic processing, a distinct advantage in the thermionic valve era due to minimal valve count and low power consumption, the instrument achieved great popularity as a portable radiation detector.

Modern versions of the Geiger counter use the halogen tube invented in by Sidney H. G-M pancake detector feeding a microcontroller data-logger sending data to a PC via bluetooth.

A radioactive rock was placed on top the G-M causing the graph to rise. Media related to Geiger counters at Wikimedia Commons.

From Wikipedia, the free encyclopedia. Instrument used for measuring ionizing radiation. Main article: Geiger—Müller tube. Use of a "hot spot" detector on a long pole to survey waste casks.

G-M counters being used as gamma survey monitors, seeking radioactive satellite debris. Radiation Detection and Measurement , third edition Retrieved Rutherford and H.

Geiger and W. Müller , "Elektronenzählrohr zur Messung schwächster Aktivitäten" Electron counting tube for the measurement of the weakest radioactivities , Die Naturwissenschaften The Sciences , vol.

Geiger, H. Physical Review. Bibcode : PhRv Geophone Hydrophone Microphone Seismometer. Air—fuel ratio meter Blind spot monitor Crankshaft position sensor Curb feeler Defect detector Engine coolant temperature sensor Hall effect sensor MAP sensor Mass flow sensor Omniview technology Oxygen sensor Parking sensors Radar gun Speed sensor Speedometer Throttle position sensor Tire-pressure monitoring system Torque sensor Transmission fluid temperature sensor Turbine speed sensor Variable reluctance sensor Vehicle speed sensor Water sensor Wheel speed sensor.

Breathalyzer Carbon dioxide sensor Carbon monoxide detector Catalytic bead sensor Chemical field-effect transistor Electrochemical gas sensor Electrolyte—insulator—semiconductor sensor Electronic nose Fluorescent chloride sensors Holographic sensor Hydrocarbon dew point analyzer Hydrogen sensor Hydrogen sulfide sensor Infrared point sensor Ion selective electrode ISFET Microwave chemistry sensor Nitrogen oxide sensor Nondispersive infrared sensor Olfactometer Optode Oxygen sensor Pellistor pH glass electrode Potentiometric sensor Redox electrode Smoke detector Zinc oxide nanorod sensor.

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