The Geiger Muller Counter is the most widespread instrument for detecting ionizing type radiation: Alfa, Beta e Gamma, of nuclear origin.
The operation of the Geiger counter is based on the principle of the Geiger Muller tube which was invented in 1913 by Hans Wilhelm Geiger and then later improved by Walther Müller.
The Geiger Counter uses the particle detector tube: Geiger Muller, which is still the most used sensor for measuring radioactivity today: Alfa, Beta e Gamma. .
Geiger Muller counters are built with different efficiency parameters, sensitivity and precision with very different costs. However, their primary function is always the same, that is, counting the number of radioactive particles that pass through them in a certain interval of time.
For example ours Geiger counters of the series “Guardian Ray Smart 7317 e Mini violin 7317 “, they use exclusively high performance Geiger Muller tubes”.
The Geiger tube works like an ion drift chamber.
The Geiger Counter works on the physical principle of the Geiger Muller tube intended as an ion drift chamber. the operating point is intentionally set at a relatively high voltage value, which however is slightly lower than what would instead cause the total ionization of the gas.
Therefore, favorable conditions have been created so that even further ionization produced by the passage of ionizing radiation in the gas no longer has to depend on the energy released by the radiation itself..
As a result, the resulting electric field to which the gas is subjected is then so intense that even the secondary ionizations created by the passage of the radioactive particles will generate further ionizations.
This phenomenon is called by physics “avalanche multiplication”, and manifests itself with a resulting electrical impulse due to the sudden change in state of the gas which from a perfect insulator becomes for a brief instant a conductor of electric charges..
The gas mixture contained in the Geiger tube is ionized by applying it to the electrodes of the probe itself, an electrical voltage high enough to generate a pre-discharge state.
As a consequence, the ionization level will be a little below the critical value which would instead cause the continuous conduction of its internal gas with a self-sustained electrical discharge.
On the other hand, if the appropriate conditions occur, the gas contained in the Geiger tube itself will be able to conduct the electric current only for very short moments., from the moment it is hit by ionizing radiation.
So that the discharge in the gas a triggered muzzle can go out very quickly, this is mixed with halogens and alcohol vapors which contribute to the function of “quencing”.
A high Electric field is applied to the Geiger tube
The so-called pre-bias voltage is not applied directly to the Geiger tube, but a resistance of very high ohmic value is interposed in series, of the order of several megohms.
This resistor basically serves to facilitate the extinction of the electric discharge in the gas after it has been crossed by an ionizing particle.
In the Geiger Muller tube there are therefore two electrodes, the resulting cathode is generally connected to the negative pole of the battery and therefore to the metal or metallized wall of the tube.
Instead the anode is a central collector, electrically isolated from the tube wall and subjected to a positive direct voltage of the order of 400 – 800V.
On the other hand, the value of the applied voltage necessary to reach the linear response zone of the tube (PLATEAU), It depends not only on the dimensional characteristics of the Geiger tube but also on the physical properties of the gas.
This voltage must absolutely be slightly lower than what continuous conduction would cause, and consequently the electric discharge in the gas due to the avalanche effect.
Therefore the electric field thus generated inside the detection device looks like this “pronto” to trigger an avalanche of electric current as soon as even a single pair of ions forms in the gas due to the radiation hitting it.
The actual sensitivity, it depends directly as well as on the applied voltage, also by size, in fact, the larger the tube, the larger the active surface is capable of receiving and therefore counting ionizing radiation with greater consistency.
Every time an energy-charged particle passes through and ionizes the gas present in the Geiger Muller tube,as a consequence, a micro electric discharge is triggered for a few microseconds which causes a small current to flow between the two power supply terminals.
The power supply voltage is applied by interposing a high-value resistor in series with the sensor power supply circuit.
So it happens that between the terminals of the Geiger tube, due to the voltage drop due to the electric discharge in the gas, a negative impulse is generated with an amplitude of approximately 5/10 volts with a duration ( of approximately 50/100 microseconds).
The ionization of the gas molecules produced by any ionizing particle passing through it would add to the already significant electric field associated with the high potential difference applied on the terminals of the Geiger counter tube
The resulting impulse does not depend on the energy released by the impacting particle, and therefore by the number of ion pairs produced.
Indeed, when it passes through the meter tube and hits the gas, one of its molecules ionizes, creating an ion-electron pair. But in these devices the collected charge is independent of the primary ionization.
The best Geiger counters made in Italy, True Italian excellence.
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