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GEIGER-MULLER TUBE
Manufacturer: Various
Cost: $100 (1980)
Description
A mica windowed, halogen quenched, GeigerMuller
radiation detector capable of detecting individual
beta particles and gamma rays when connected to an
appropriate power supply and electronic pulse counter.
Specifications
Mica window density | 1.4 - 2.0 mg/cm squared |
Plateau voltage | ~ 950 volts |
Plateau length | greater than 200 V |
Plateau slope | less than 10%/100 V |
Dead time | ~ 200 us |
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Operating Instructions
- The tube is to be operated in the housing supplied, in
order to protect the window, and the assembly
connected to a Picker Nuclear Compact Scaler. Samples
can be placed in pans or other appropriate containers
and inserted in the housing at set distances beneath
the window. Absorbers can also be inserted between
the sample and the tube.
- Before conducting any measurements the correct
operating voltage of the G-M tube should be
determined. Set up a moderately weak source (use the
nominal voltage on the tube to determine this) under
the tube and repeatedly count it while changing the
high voltage. Start at about 700 V and work up first
in 50 V and later in 20 V steps until the count levels
off to about a 10%/100 change. Plot a graph as you
go. Keep increasing the voltage until the count
begins to increase again significantly. DO NOT GO TO
HIGHER VOLTAGES. The optimum operating point is about
1/3 of the way from the bottom of the plateau to the
top.
Principles of Operation
The tube contains gas at a low pressure (~ 2 Torr).
When a beta particle or gamma ray passes through it, a trail
of ionized atoms will be left behind. (alpha particles will
ionize effectively but cannot usually penetrate the window.
gamma rays can enter through the window or the walls). The
charged ions will be accelerated strongly to one or other
electrode and will further collide and produce more ions.
In this manner the originally small number of ions is
greatly multiplied, and when they are finally collected at
the electrodes an easily measurable pulse of current is
drawn from the high voltage supply. The presence of a small
quantity of a halogen element aids in stopping the
multiplication process promptly after each excitation.
Because the multiplication process proceeds to a saturation,
(approx 10 to the 10 ions) each time it is excited (if the
high voltage is in the plateau region) it is not possible to
tell the energy or nature of the ionizing beta or gamma.
Likewise, simultaneous passages of two or more particles
will produce only a single current pulse.
Precautions
- Do not let anything touch the window. It is very
fragile.
- Do not ever apply a high voltage beyond the plateau
region, as the tube will be damaged.
- Count rates of more than 100000/min will likely be
subject to some coincidence error (see below).
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keywords: nuclear measurement device, nuclear detector, gamma ray measurement device, gamma ray detector, nuclear detector.
Document created Circa 1970. Original author: Unknown.
Last updated 06/27/96. Revised by David Harrison.