RADIAC stands for RAdiation
Detection, Indication And Computation. All parts of the UK civil
defence services, during the Cold War, were required to be able to
measure and interpret radiation measurements. As their roles differed
somewhat the equipment they used varied a little, and also changed
during the Cold War period. A variety of scientific units of
measurement were used at different times, often in an imprecise
manner, hopefully this page will help to straighten things out.
Measuring Radioactivity
Ionizing radiation is measured in terms of:
the strength
or radioactivity of the radiation source,
the energy
of the radiation,
the level of
radiation in the environment, and
the
radiation dose or the amount of radiation energy absorbed by the
human body.
From the point of view of civil
defence, the radiation dose is the most important measure. The risk of
radiation-induced diseases depends on the total radiation dose that a
person receives over time.
Ionizing radiation can be measured using units of electron volts,
ergs, and joules. The electron-volt (abbreviated eV) is a unit of
energy associated with moving electrons around. An electron is
'tightly bound' in a hydrogen atom (one proton and one electron). It
takes energy to move this electron away from the proton, in fact it
takes 13.6 electron-volts of energy to move this electron completely
away from the proton. When that happens we say that the atom is
'ionized'. In the jargon, the 'ionization energy' of the tightly bound
electron in hydrogen is 13.6 electron volts.
Electrons have a very small mass, so we don't expect an electron-volt
to represent very much energy. One electron-volt is only 1.6 x 10-19
joules of energy, in other words, 0.16 billion-billionth of a
joule. One joule (abbreviated J) is equivalent to the amount of energy
used by a one-watt light bulb lit for one second. The energy
associated with the radioactive decay ranges from thousands to
millions of electron-volts per nucleus, which is why the decay of a
single nucleus typically leads to a large number of ionizations.More
information about radioactivity can be found on the Radiation
page.
RADIAC Equipment
The civil defence services in the UK
were issued with broadly similar equipment, with additional specialist
equipment for Royal Observer Corps posts. Additionally, because the
majority of the organisations were disbanded in 1968, the ROC had
equipment that did not see service in the Civil Defence Corps and AFS,
simply because it was not introduced until the early 1980s.
Equipment can be divided into a number of groups, based upon their
roles:
Personal
dosimetry
Contamination detection
Radiological
survey
Remote
monitoring
Personal dosimetry
All personal dosimetry for the civil
defence services utilised the same type of device, namely the
quartz-fibre dosimeter, sometimes referred to simply as the personal
dosimeter. This type of device has a number of advantages over others:
First it is
robust, it is actually very difficult to damage one, except by
exposing it to high temperatures, or high impact levels.
It needs no
special equipment or personnel to read it.
It needs no
batteries or other consumables (some reader/charger units are
battery powered).
It is
extremely simple to use, thirty minutes group training is more
than adequate.
It gives an
immediate reading.
The quartz-fibre dosimeter was in
fact used by the USA, Soviets and Chinese as well during the cold war.
UK issued dosimeters had an aluminium barrel. Early issue devices did
not have the bellows or retracting charging pin, instead they had a
removable rubber cap with a clear window. Later versions had removable
protective covers made out of soft plastic.
The quartz fibre dosimeter works by measuring the decrease in
electrostatic charge on a metal conductor in an ionization chamber,
due to ionization of the air in the chamber by radiation. It was
invented in 1937 by Charles
C. Lauritsen.
The dosimeter must be periodically recharged. It is usually read
before it is charged, and the dose is logged, to chart one's
exposure. Magnifying lenses, forming a low-power microscope, and
an illumination lens allow one to directly read the dose at any time
by aiming the illumination lens at a light source and looking into the
device
The device is mainly sensitive to gamma and x-rays, but it also
detects beta radiation above 1 MeV. It consists of a sealed air-filled
cylinder called an ionization chamber. Inside it is a metal electrode
strip that is attached to a terminal on the end of the pen for
recharging. The other end of the electrode has a delicate gold-plated
quartz fibre attached to it, which at rest lies parallel to the
electrode. The ends of the chamber are transparent and the microscope
is focused on the fibre.
Units with larger ranges had a capacitor attached between the
electrode and the case. The capacitor stores a larger amount of charge
on the device for a given voltage on the electrode. Since each
radiation particle allows a fixed amount of charge to escape, a larger
number of radiation particles is required to move the fibre a given
amount.
During charging, the charger applies a high DC voltage, usually around
150-200 volts, to the electrode, giving it an electrostatic charge.
The quartz fibre, having the same charge, is repelled by the surface
of the electrode due to the coulomb force and bends away from the
electrode. After charging, the charge remains on the electrode because
it is insulated.
When a particle of ionizing radiation passes through the chamber, it
collides with molecules of air, knocking electrons off them and
creating positively and negatively charged atoms (ions) in the air.
The ions of opposite charge are attracted to the electrode and
neutralize some of the charge on it. The reduced charge on the
electrode reduces the force on the fibre, causing it to move back
toward the electrode. The position of the fibre can be read through
the microscope. Within the device is a transparent scale marked with
the required units, known as the graticule.
Since each radiation particle allows a certain amount of charge to
leak off the electrode, the position of the fibre at any time
represents the cumulative radiation that has passed through the
chamber since the last recharge. Recharging restores the charge that
was lost and returns the fibre to its original, zero, deflected
position.
Various kinds of charger have been developed. In the UK, they were of
two broad types. The first types issued used a hand generator similar
to an old-fashioned telephone magneto. Later types used a single
transistor inverter circuit powered by a D-type cell. Whilst the
former types relied on a mirror reflecting ambient light up the
dosimeter bore, later types included a small light bulb for
illumination.
One training and three operational versions were issued to the Civil
Defence Corps, WRVS and AFS
with the following ranges:
Training (No. 1) reading
0 - 0.5r.
Operational (No. 2) reading 0 - 5r
Operational (No. 3) reading 0 - 50r
Operational (No. 4) reading 0 - 150r
The Royal
Observer Corps were issued with three versions with the
following ranges:
Type No. 1 measuring 0 - 0.5R. They
were sometimes marked with a black identification band, and were
often called the Training Type Individual Dosimeter.
Type No. 2A measuring 0 - 5R. Identified by a
blue band.
Type No. 3 measuring 0 - 50R.
Identified by a red band.
The dosimeter shown is of the
earliest issue, they can be distinguished by the black rubber cap
covering the charging pin, and the fact that they do not have an
internal protective bellows. Early models of charger had a device for
removing the rubber cap.
Personal dosimeter chargers
The first model of Dosimeter
charger/reader issued to the civil defence services, and dates from
about 1950. The Charger dosimeter No1 is operated by a hand generator,
and reading is by way of ambient light reflected from a built-in
mirror. The intention was for these to be placed at fixed points, e.g.
sector warden posts, ROC posts and the like. The earliest issue had a
device fitted to the top to enable the removal of the black protective
cap from dosimeters, the later version omitted this. Winding the
handle generated an AC voltage which was rectified by a selenium
rectifier, which in turn charged a capacitor. A small amount of charge
was then transferred from this capacitor to a 1nF capacitor by means
of switch 2, and thence to the output capacitor. Switch 2 was operated
by a thumbwheel.
Charger, Dosimeter No 2 Mk 2
The No 2 Mk 2 model was similar in
use to the No 1. Additions included a carrying strap and a socket
cover. I never saw the purpose of the carrying strap. It was still
available in the period 1964-8, as was the No 1. The actual circuit
was pretty much identical to that of the No1 charger, but arranged
differently in physical terms and with a two way charge/discharge
switch. Again the first part of the instrument was a hand operated
alternator, the output of which was used to charge a capacitor via a
selenium rectifier. The charge was then switched via another pair of
capacitors and a high value resistor to the charging socket. Light was
still deflected up the dosimeter by way of a Mirror. The No 2 Mk 1 had
a flat metal cover for the charging socket, this was an incomplete
answer to contamination of the socket and interior of the device, it
was replaced by a rubber stopper in the Mk 2. The No 1 and No 2 Mk 2
were succeeded by a battery operated device in about 1968. This latter
was issued in small numbers to the Civil Defence Corps.
Electronic dosimeter chargers
The Type N.105A was the most
common used by the Royal Observer Corps. There is some evidence
that another model by R. A. Stephen in Mitcham, Surrey, the P1548 was
also issued, but I have been unable to confirm this. The P1548 circuit
was identical to that of the N.105.A. The N.105.A used by the Royal
Observer Corps, was introduced in 1967. It used a single germanium
transistor circuit powered by a single U2 cell. In fact by the time it
was introduced the transistor was already obsolete! Included was a
small filament bulb to illuminate the scale of the dosimeter. Both of
these battery operated devices had significant advantages over the
earlier models. They were much lighter, less susceptible to internal
contamination , did not need ambient light to read the dosimeters, and
were easier to use when setting the fibre position. The only
disadvantage was the need for a battery, but these were easy to obtain
for local replacement. The Civil Defence Corps were due to have
been issued a similar charger at the time of disbandment.
The switch is part of the charging socket, inserting the dosimeter
turns the charger on, illuminating the scale, however the charging pin
is not connected. This means the dosimeter can be read without
re-zeroing it. Depressing the dosimeter further connects the pin, and
it is then possible to zero it. Unlike the previous chargers the
zeroing is continuously variable which makes it much easier to use.
The user needs to be careful not to over depress the dosimeter
otherwise there is a serious risk that the current reading may be
changed or even cancelled.
Two other types of radiation measuring instruments were used in civil
defence during the cold war, technically they were either ionisation
chamber meters or Geiger counters. Ionisation meters and Geiger
counters differ in their modes of operation, both of which are
explained below.
Ionisation chamber instruments
An ionisation chamber is a gas
filled container, it detects radiation by measuring a voltage between
two electrodes created by the flow of ions generated by radioactive
particles, gamma or X-rays. Civil defence ionisation instrument
chambers contain dry air at atmospheric pressure. Two electrodes, with
a voltage (typically 15-100V), known as the polarising or bias
voltage, across them form an electric field, and in the presence of
ions in the chamber cause a flow of electric current between them.
This flow is usually very small, in the femtoampere (one femtoampere
is a billionth of a millionth (10-15) of an ampere) range, and
detectable by electronic means.Survey meter simplified circuit
The chamber may be any shape with one electrode, the anode,
consisting of either a simple rod or a flat plate. The wall of
the chamber is usually metal and serves as the cathode connected to a
negative potential. A large potential between the electrodes
establishes an electric field between the two. The field is strong
enough to pull the ion pairs, however not so strong that it creates
further ions. In some cases the chamber has a thin wall made of some
form of plastic.
When energetic radiation in the form of particles such as alpha, beta,
or gamma rays interacts with the atoms of gas that that fill the
chamber, they will either lose an electron or gain an electron. When
an atom loses an electron, its overall charge becomes positive and
therefore the cathode end of the chamber attracts it. However, when an
atom gains an electron, its overall charge becomes negative and
therefore the anode end of the chamber attracts it.
The flow of these ions therefore constitutes a flow of electron charge
proportional to the amount of ions present. The flow of charge within
the circuit is minute, this means an amplifier is utilised to make
this tiny change more apparent.
Both the Meter Doserate Portable No1 and the Meter Survey Radiac No 2
were built by E.K.Cole Ltd. of Southend-on-Sea, perhaps better known
for the manufacture of radios and televisions under the brand name
Ekco. E.K.Cole Ltd had been founded in 1924 by Eric Kirkham Cole and
his girlfriend Muriel Bradshaw.
Meter Doserate Portable No 1
The Meter Doserate Portable No 1 had
a single range of 0 - 3 r.p.h. This is an ionisation type meter and
not a geiger counter. It was replaced with the No 2, because its
single range was far too narrow for wartime use, consequently there
are very few still in existence. This should not be confused with the
Meter Doserate Portable No 1 Trainer, see above.
The batteries comprised a pair of D cells and another obsolete
HT battery. One D cell supplied the scale lamp, and the other the
filament current for the electrometer valve. The D cells are contained
behind the large circular covers, and CD personnel were permitted to
change these. In the event of a spurious reading or a low battery test
reading, the unit was meant to have been returned to the Servicing
Department for testing and replacement of the HT batteries. These
latter could be reached by removing the battery container, using the
four screws around the D cell covers. In the front end, below the
meter there was a humidity detector, which changed colour in the
presence of moisture, if this happened the meter became inaccurate and
again had to be returned.
Meter, Survey, Radiac, No. 2
The Meter Survey Radiac No 2 is
commonly sold on ebay and other sites as a geiger counter which it is
not! These, again, are ionisation type meters intended for measuring
fallout from nuclear attack. They will not measure, or even detect
low-level radiation. If you get a reading on one, except in nuclear
war conditions, or close in to a major nuclear incident (metres) then
your meter is faulty!
The dose-rate in Roentgen-hour (R/hr) is indicated on a direct reading
meter with a linear scale. Three ranges are provided, 0-3R/hr,
0-30R/hr, 0-300R/hr. A moving scale on the meter is mechanically
linked to the Range Switch to indicate the range in use . The
ionisation chamber used has an air equivalent wall and the calibration
is Independent of gamma energy, within 10%, over the energy
range O.l - 1.0 MeV.
The instrument may be made sensitive to beta radiation by the
removal of a panel which is normally screwed to the base of the
instrument. A hinged flap and beta window assembly can be opened when
the base panel is removed. When the beta flap is open, beta
particles of energy greater than about 0.4MeV can penetrate to
the ionisation chamber detector element.
The operational controls are situated on the side of the
instrument. When used for gamma measurement the instrument may
be carried in its haversack, access to the controls is then obtained
through a flap on the side. The ON/ OFF switch operates a flag on the
meter to indicate the position of this switch. The meter scale can be
illuminated by a lamp for use when the instrument is operated in the
dark. This instrument weighed about 6 lbs.
In addition to the two D cells required for the valve (tube) filament,
and the meter lamp, this instrument required HT 9 volt and 30 volt
batteries which were obsolete when the unit was introduced and had to
be made to special order.
Meter Survey Lightweight (AVO
RADIAC Meters)
This was the smallest and lightest
ionisation Survey Meter issued to the civil defence services. As far
as I am aware it was not issued to the Civil Defence Corps, although I
did see one during training, recently acquired evidence shows that at
least some county authorities had these meters in 1961. During
training we were told that they were to be issued to the ROC only. The
Survey Meter, Lightweight was built by the AVO company. The Mk 3 was
first issued in about 1960 and had a logarithmic scale reading
0-100RPH. I can find no references to its use, but understand it was
not popular due to reliability issues, the Meter Survey Radiac No 2
was much preferred, despite the fact that it weighed some three or
four times as much. The first issue I can find reference is to the No
1 dating from the late 1950s. The last issue appears to have been of
the Mk 6, which was the last issue prior to the PDRM 82 in 1982.
Apparently these were only issued to ROC sector and group controls.
The unit was provided with a neck strap but without any form of cover.
Fixed Survey Meter
The early model of the Fixed Survey
Meter (FSM) was used by the Royal Observer Corps from the early 1950s
until 1982/3, it was designed by the Atomic Weapons Establishment at
Aldermaston and built by AVO, after that date the PDRM82F was
used. The FSM was not used by other services. The PDRM82F was also
referred to as the FSM in the training literature as it performed the
same function. As the PDRM82F was a true geiger counter it is
considered further below.
Prior to the introduction of the FSM it was necessary for a post crew
member to leave the relative safety of the underground post to take
readings on the surface using a Meter Doserate Portable No1 or a Meter
Survey Radiac No2. This was a hazardous operation in the event of
fallout, and required de-contamination on re-entry to the post.
The FSM was battery operated, and had one fixed logarithmic scale from
0 to 500R/hr, which could be extended by the simple expedient of
lowering the probe into a shielded position once it reached close to
full-scale. It would read as low as 0.1R/hr at the bottom end of the
scale.
The meter was connected by a co-axial cable to an ionisation chamber
mounted onto a telescopic rod that was fed up a probe pipe in the
ceiling of the monitoring post so that the probe was above ground. The
top of the probe was protected by a polycarbonate dome that prevented
fallout from entering the post.
The instruments were kept at the group controls in an air conditioned
and de-humidified storage room and only issued to posts during
Transition To War. Once at the posts the instrument was unpacked from
its wooden transit case and prepared for use.
If radiation readings approached the 400R/hr level the telescopic rod
was quickly collapsed and the probe reinserted to a distance below the
surface that reduced the dial reading by a factor of ten. Thus the
instrument became capable of producing accurate readings to a level of
5,000 roentgens per hour external reading. When reporting readings in
the lower position this was signified to group control by prefixing
the reading with word "RED". Once the level reached 400R/hr again, the
probe was re-inserted to its full height.
Upon the first reading being received, this was reported to Group
Control as "First Fallout", subsequent readings were reported as
requested by Group. The FSM
was replaced by the PDRM82(F) in 1982/3, this was a true geiger
counter, and is described below.
The FSM was replaced by the PDRM82(F) in 1982/3, this was a true
geiger counter, which is described below.
A Geiger counter consists of a
Geiger-Muller tube and associated electronics.
Geiger tube operation
The Geiger-Muller tube consists of a
sealed metallic or glass tube filled with argon or a mixture of noble
gases mixed with a small amount of an organic gas or halogen gas. The
noble gas is called the detecting gas whereas the halogen or organic
are referred to as the quenching gas. The gas mixture inside the tube
is at a pressure below atmospheric. A metal wire or rod runs through
the centre of the tube, and is known as the anode. Either the metallic
tube, a metallic cylinder or a conductive film lining the inner of the
glass tube, in the case of a glass tube, forms the cathode. An
electric potential of up typically 350-1500 volts is maintained
between the anode and the cathode. In the absence of any radiation no
current flows between the wire and the cylinder.
When a radioactive particle, gamma or X-ray enters the tube it ionises
an inert gas atom, releasing an electron. The resulting electron is
accelerated towards the metal wire or anode.
As the electron approaches the metal wire it experiences an increasing
electric field strength which in turn applies a greater accelerating
force on the electron. The accelerating force becomes so strong that
on collision with other argon atoms the electron can ionise them,
releasing further electrons, generating a cascade of further
electrons, an effect called the avalanche or Geiger effect. The
ionisation by one particle can result in millions of electrons
striking the metal wire. This only occurs within a limited range of
applied voltages, known as the plateau region. In the centre of this
range is the working voltage, for UK civil defence instruments this is
in the range of 350-500 volts, on the larger tubes this value is
typically marked on the tube itself. The avalanche produces a pulse
for each original ionisation. Pulses are of equal amplitude, and the
number of pulses indicates the number of events rather than the energy
of the individual particles or gamma radiation.
The purpose of the quenching gas is to absorb the positive noble gas
ions as they accelerate to the cathode. Without the quenching gas
these positive ions will be neutralised at the cathode in an exited
state or could even also dislodge electrons from the cathode. These
dislodged electrons or excited atoms could trigger further ionisation
creating a further voltage discharge giving inaccuracies in the
measure from the device. When the quenching gas migrates to the
cathode it recombines at ground state and so does not present the
potential to cause any further ionisation. Some early UK tubes used an
organic quenching gas, most later tubes contained bromine.
Special tubes were available for different purposes. For counting
alpha radiation a special thin mica window is inserted in the end of a
tube, no UK civil defence instruments were of this type. The
CV2287 was used in the Meter Portable Training, it was sensitive
to both high energy beta radiation and to gamma, but the metal case
made the instrument only sensitive to gamma. The CV2246, CV2247,
CV2248 were used in the Contamination Meter No 1 Mk1 and 2. The first
two are sensitive to high energy beta particles and to gamma rays. The
CV2248 has a glass well and was used for measuring radioactivity in
liquids. The ZP1301 was fitted to the PDRM 82 and the PDRM 82F. It is
a specially compensated tube that is only sensitive to gamma radiation
above a certain energy. This latter tube, the ZP1301, also had an
inbuilt radioactive check source. The initial issue only had a half
life of just over ten years, later issues had a different isotope with
a half life of 27 years. The later tubes can be identified by a small
radiation trefoil label, some PDRM82s were also fitted with a later
type tube from the same series.
Meter Doserate Portable No 1
Trainer
The purpose of the Meter Doserate
Portable No 1 Trainer was to train personnel in the use of the Meter
Doserate Portable No 1 (later also used for the No 2). Note the Geiger
Muller tube at the bottom. This instrument used valve (tube)
technology, with a D cell to provide the filament current, and HT
batteries which were already obsolete by the time the instrument came
into use and had to be made to special contract by Ever Ready.
The geiger-muller tube is a CV2287 which is both large and sensitive.
This tube is sensitive to hard beta radiation, the trainer itself is
only sensitive to gamma radiation because of the thick-walled metal
case. Although not intended for operational use it is a completely
functional instrument, and could have been used as a contamination
meter, although this purpose is not described in any of the civil
defence literature or training manuals. It has a single range reading
0 - 300 microroentgens per hour. Meter illumination was by a small
neon bulb. It was used by the military, Civil Defence Corps, Royal
Observer Corps and the Auxiliary Fire Service.
Meter, Contamination No1
The Meter, Contamination No1 was
issued in two variants, the No1 Mk1 and No1 Mk 2, the Mk1 had metal
plugs for the probe, the Mk2 rubberised. It was a true Geiger
counter that could be fitted with several different tube types.
Contamination Meter No. 1Three different power supplies were
available. The Battery Holder No1 was fitted with two 150 volt
batteries. The Power Unit, Vibrator No1 used four 1.35 volt mercury
cells. The Power Unit, Mains No 1, could operate from 100-120 volts or
200-250 volts ac, 50-60Hz. The latter unit is potentially lethal, as
if it is plugged into the mains and not into the counter there are
prongs exposed at mains potential.
The controls were all on the top of the instrument, they comprised an
on/off switch, headphone socket, meter, test switch, a connector for
the probe, and two preset controls "A" and "B". Headphones were not
issued to the civil defence services. The meter is roughly logarithmic
and reads 0 to 10mR/hr. Preset control A is used to set the tube
working voltage which needed to be done in a properly equipped
workshop. Preset control B is used to set supply voltage if on test it
reads outside of the correct range.
PDRM 82
The PDRM 82 was designed for
simplicity in operation, and was introduced to the ROC in 1982,
roll-out being completed by 1985. It was also issued to the fire
service and emergency planning officers. The PDRM 82 is a portable,
lightweight, water resistant gamma radiation survey meter to measure
radiological dose rate in the range 0.1 to 300 centiGrays per hour in
air. The Geiger Muller (G.M.) tube detecting unit is energy and polar
response corrected. This unit comes with a plastic neckstrap and a
waist lanyard. If, when switched on, the unit shows "FAIL", and
does not clear within 1 minute, then it is faulty. The most probably
cause of this is either the unit is damp internally, or the tiny
amount of radioactive isotope that forms part of the GM tube self test
is too weak, the half-life of the isotope used is 10 years, 27 years
or 30 years depending on which tube has been fitted, and the tube will
need replacing (expensive). No routine maintenance is required
or possible except for the replacement of the 3 'C' cells. It has a
large LCD display with a range of 0 - 300 cGy/h. The unit has a
battery life of about 400hrs.
It is possible to modify the PDRM 82 to make it considerably more
sensitive (about 1000x) by replacing the geiger tube at a cost of
about £10-15, or to possibly re-activate a non-functioning unit. For
details of the modification click here.
PDRM 82F
The PDRM82F is almost identical in
appearance to the PDRM82, and shares virtually all of its
circuitry.The most obvious differences are the bnc type socket on the
rear and the external probe to which it connects via a coaxial cable.
The PDRM82F replaced the earlier Fixed Survey Meter in the Royal
Observer Corps starting in 1983, with roll-out completed by 1985. Its
purpose was the same as that of the FSM, and in training materials the
term FSM continued to be used. The external probe contained the same
type of tube as the portable model. The display remained on the
instrument table, and the probe was pushed up the ceiling mounted pipe
in the monitoring room, and into the external plastic dome. To
increase the range of reading, if the reading due to fallout
approached 300cG/hr, then the probe would immediately be lowered to a
more shielded position so that it gave 1/10 of the reading, and be
clamped in that position.