DOE-HDBK-1122-99 Module 2.16, Fundamental Academic Training Instructor's Guide Phase I; Module 2.16, Radiation Survey Instrumentation
Functional areas: Radiological Control, Technician Training, Instructor's Guide, Radiation Survey, Instrumentation
External exposure controls used to minimize the dose equivalent to personnel are based on the data taken with portable radiation survey instruments. An understanding of these instruments is important to ensure the data obtained is accurate and appropriate for the source of radiation. This lesson contains information about widely used portable
radiation survey instruments.
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Section 1
DOE-HDBK-1122-99
Module 2.16 Radiation Survey Instrumentation Instructor’s Guide
2.16-1
Course Title: Radiological Control Technician
Module Title: Radiation Survey Instrumentation
Module Number: 2.16
Objectives:
2.16.01 List the factors which affect an RCT's selection of a portable radiation
survey instrument, and identify appropriate instruments for external
radiation surveys.
� 2.16.02 Identify the following features and specifications for ion chamber
instruments used at your facility:
a. Detector type
b. Instrument operating range
c. Detector shielding
d. Detector window
e. Types of radiation detected/measured
f. Operator-adjustable controls
g. Markings for detector effective center
h. Specific limitations/characteristics.
� 2.16.03 Identify the following features and specifications for high range
instruments used at your facility:
a. Detector type
b. Instrument operating range
c. Detector shielding
d. Detector window
e. Types of radiation detected/measured
f. Operator-adjustable controls
g. Markings for detector effective center
h. Specific limitations/characteristics.
� 2.16.04 Identify the following features and specifications for neutron detection and
measurement instruments used at your facility:
a. Detector type
b. Instrument operating range
c. Types of radiation detected/measured
d. Energy response
e. Operator-adjustable controls
f. Specific limitations/characteristics.
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References:
1. Radiation Detection and Measurement, Glenn F. Knoll
2. Basic Radiation Protection Technology, Daniel A. Gollnick
3. Operational Health Physics, Harold J. Moe
4. ANSI N323A
5. (Various Manufacturers Technical Manuals)
Instructional Aids:
1. Overheads
2. Overhead projector and screen
3. Chalkboard/markerboard
4. Lessons learned
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I. MODULE INTRODUCTION
A. Self Introduction
1. Name
2. Phone number
3. Background
4. Emergency procedure review
B. Motivation
External exposure controls used to minimize the dose
equivalent to personnel are based on the data taken with
portable radiation survey instruments. An understanding of
these instruments is important to ensure the data obtained is
accurate and appropriate for the source of radiation. This
lesson contains information about widely used portable
radiation survey instruments.
C. Lesson Overview
1. General discussion
2. Factors affecting instrument selection
3. Eberline RO-2 series
4. Bicron RSO-50 and RSO-500
5. Victoreen 450B
6. Eberline Teletector
7. Eberline RO-7
8. Eberline PNR-4 with NRD sphere
9. Eberline ASP-1 with NRD sphere
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D. Introduce Objectives Show O.H.: Objectives
NOTE: The text is
provided for some
commonly used
instruments. The
facility must adjust text
as necessary for
instruments used at
each site. Text added
for specific instruments
used at the facility
must, at a minimum,
cover material required
by the objectives.
II. MODULE OUTLINE
A. General Discussion
1. Measurements using portable radiation survey instruments
provide the basis for assignment of practical external
exposure controls. In order to establish the proper
controls, radiation measurements must be an accurate
representation of the actual conditions.
2. Many factors can affect how well the measurement
reflects the actual conditions, such as:
Section 2
a. Selection of the appropriate instrument based on type
and energy of radiation, radiation intensity, and other
factors.
b. Correct operation of the instrument based on the
instrument operating characteristics and limitations.
c. Calibration of the instrument to a known radiation
field similar in type, energy and intensity to the
radiation field to be measured.
d. Other radiological and non-radiological factors that
affect the instrument response, such as radioactive
gases, mixed radiation fields, humidity and
temperature.
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B. Factors Affecting Instrument Selection Objective 2.16.01
1. As discussed, the selection of the proper instrument is
critical to ensure the data obtained are accurate and
appropriate.
2. The instrument is selected based on the characteristics and
specifications for that instrument as compared to the
required measurements.
3. Several factors should be considered when selecting the
instrument.
a. Type of data required:
Distinguish clearly between external radiation surveys
(lesson 2.16) and contamination monitoring (lesson
2.17). External radiation surveys require an instrument
that reads R/hr, rem/hr, etc, rather than cpm, etc.
b. Measurement of the true dose equivalent:
Ion chambers (which read current instead of counting
pulses) have the flattest energy response. Ion
chambers are closest to being tissue equivalent.
Generally the best choice for external beta-gamma
surveys is an ion chamber.
c. The type of radiation to be measured:
Ion chambers measure beta and gamma;
For neutrons, choose a rem ball (NRD);
Alphas are not measured in an external radiation
survey, since they do not penetrate the skin (7
mg/cm2).
d. The intensity of the radiation (exposure or dose rate):
For high radiation fields (> 5 R/hr) use an extendible
instrument (Teletector) if this is "reasonably
achievable" (ALARA).
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e. The energy of the radiation to be measured:
low energy radiation will not penetrate either the skin,
or the window of most external radiation instruments;
GM detectors over-respond to low energy gammas;
most instruments under-respond to high energy
neutrons.
f. Environmental factors:
ion chambers are usually vented to air, so radioactive
gases or high humidity affect the instrument response
g. Procedural requirements
4. Pre-operational check.
Once the proper type of instrument has been identified, a
pre-operational check is essential and must be performed
in accordance with appropriate procedures.
a. Physical damage
Perform a physical inspection of the instrument by
checking for obvious physical defects or damage,
especially of the probe, and replace the probe or cable
if necessary.
b. Calibration
Verify the instrument is calibrated and has not
exceeded the calibration due date.
c. Battery
Perform a battery check to verify the battery condition
is within the acceptable range. Change the batteries if
necessary.
d. Zero
Perform a zero adjustment for the meter needle, if
applicable.
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e. Source check
Perform a source response check as required by
procedures.
5. To ensure the proper selection and operation of
instruments, the instrument operator must understand the
operating characteristics and limitations of each
instrument available for use.
Section 3
The following general principles apply to each of the
specific instruments described in later sections.
a. Detector type.
Ion chambers have the flattest energy response. Ion
chambers are closest to being tissue equivalent.
GM detectors over-respond to low energy gammas.
Special detectors are used for neutrons.
b. Operating range.
External radiation measuring instruments read in R/hr,
rad/hr, or rem/hr. In contrast, instruments designed
for measuring contamination read in cpm.
Extendible instruments are generally appropriate for
high radiation fields.
c. Detector shielding.
Large amounts of shielding are not practical with a
portable instrument, but some probes incorporate a
small amount of shielding to reduce background.
Many external radiation survey instruments
incorporate a sliding "beta shield". Note that this also
shields low energy gammas.
d. Detector window.
External radiation instruments generally have
windows that are about as thick as human skin
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(7mg/cm2). The reason for this is: if the radiation does
not penetrate this window then it does not penetrate
skin, and so it does not contribute any external dose.
In contrast, contamination monitoring instruments
have thinner windows.
e. Types of radiation detected/measured.
Ion chambers have a flat energy response for gammas.
Ion chambers are closest to being tissue equivalent.
They are also good for betas, but a correction factor
may be needed.
Tube shaped GM detectors are designed so that the
walls are close to the detector gas. Gamma
interactions in the walls are important. A well
designed detector wall can partially compensate for
the over-response to low energy gammas. They are
designed primarily for gammas, and also measure
betas if the window is not too thick.
Pancake shaped GM detectors have side walls
separated from the gas. They are good for betas, but
have a low efficiency for gammas because very few
gammas hit the side walls.
Gas proportional detectors distinguish between alphas
and betas. They often discriminate against (reject)
betas and gammas.
ZnS scintillation detectors only detect alphas.
NaI scintillation detectors are generally used for
gammas.
Neutron detectors are very specialized.
f. Operator adjustable controls.
Portable instruments generally have a battery check.
Ion chambers generally have a zero adjustment.
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g. Markings for effective detector center.
External radiation surveys are generally taken at 30
cm (except for transportation, see lesson 2.12) It is
not always obvious what point on the detector should
be 30 cm from the source, so most detectors mark the
effective center.
1) The effective center of the detector, as defined in
ANSI N323, is the point within the detector that
produces, for a given set of irradiation conditions,
an instrument response equivalent to that which
would be produced if the entire detector were
located at that point.
2) The effective center can be thought of as the point
in the detector where the measurement of the
radiation intensity is taken.
3) Portable radiation survey instruments are
calibrated in a uniform field of radiation larger
than the volume of the detector, so that the same
radiation intensity is seen throughout the detector.
4) Therefore, the reading "taken" at the effective
center represents the rate value in all portions of
the detector.
Section 4
5) If the radiation field over the whole detector is not
uniform (such as from surface contamination,
radiation streaming, or from a small point source)
the exposure rate will not be uniform over the
entire detector volume.
6) For non-uniformly irradiated detectors, the
displayed value, as "taken" at the effective center,
will not reflect the actual exposure rate value and a
correction factor may be needed.
C. Eberline RO-2 Series Instruments Objective 2.16.02
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1. The Eberline RO-2, RO3 series of instruments are
portable, air-vented ion chamber instruments used to
detect and measure gamma, X-ray, and beta radiation.
Show actual
instruments
Technical specifications for the RO3 are similar to the
RO2.
2. Detector
a. Operated as an ionization chamber Show actual detector
with desiccant pack
b. A phenolic, or plastic, cylinder of 3 in. diameter and
12.7 in3 (208 cm3 volume with one end open but
covered by a Mylar window)
c. Fill gas - air (vented to atmosphere through a
desiccant pack)
d. The ion chamber detector is closer to tissue-equivalent
than most types, allowing the instrument to accurately
access the exposure rate to human tissue.
1. The detector is approximately tissue equivalent
because the materials used for construction have
an effective atomic number Z close to that of
tissue at 7.5.
2. Tissue equivalent implies that the detector
responds the same as human soft tissue (muscle)
would if placed at the same point in the radiation
field.
No detector is perfectly "tissue equivalent", but a
well-designed Ion chamber is close enough for
most work.
e. Although the detector is not as sensitive as a GM, it is
the detector of choice for accessing exposure because
of its close correlation to the energy deposited in
human tissue by radiation.
3. The RO-2 series instruments are operated in the current
mode, or the mode that averages the individual pulse
heights per unit time.
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a. Individual pulse information is lost; therefore, the
electrical signal will not supply information about the
type and energy of the individual radiation
interactions.
b. However, small pulses, which would be lost in the
pulse mode, are averaged along with the other
interactions.
4. The instrument range of the Model RO-2 is 0 to 5000
mR/hr.
The readings are expressed in R since the measurement is
made in air.
The settings are as follows:
RO-2 Ranges:
0-5 mR/hr
0-50 mR/hr
0-500 mR/hr
0-5,000 mR/hr
5. The sliding beta shield is made of phenolic as follows: Review the concept of
density-thickness if
necessary
• RO-2 shield: 400 mg/cm2 (1/8 inch) mounted on
case.
• The active volume of the detector is shielded from the
side by the detector wall and the instrument case, and
from the bottom by the movable beta shield and two
layers of windows.
• Detector wall is 200 mg/cm2 and the 0.13 cm
aluminum case is about 345 mg/cm2.
6. The materials and density-thickness value of the two
windows, one on the case and one on the detector, for the
Model RO-2 and RO3 are as follows:
Show windows on
instruments
• RO-2 windows: 7 mg/cm2 total, two Mylar windows
of 3.5 mg/cm2 each.
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• RO-3 windows: 3.5 mg/cm2 total, one window of 1
mil Mylar.
Section 5
7. The Model RO-2 instrument is designed to measure
gamma, x-ray, and beta radiation but will detect (not
measure) fast neutron radiation.
a. The instruments will read approximately 10%, in
mR/hr, of the true neutron field, in mrem/hr.
b. Although an ionization chamber would respond to
alpha radiation, the Mylar windows and the air gap
between the two windows eliminates any possibility
of an alpha response.
8. The energy response for the Model RO-2 is as follows:
a. Measures photon radiation within +20% for photon
energies from 12 keV to 7 MeV (beta shield open).
The minimum energy increases to 25 keV if the shield
is closed, and to about 40 keV through the side of the
instrument.
Because of the thinner window, the RO3 measures
photons from 8 keV.
b. Measures beta radiation >70 keV with the beta shield
open. A beta factor may be appropriate for some
situations.
9. Operator-adjustable controls
a. RO-2 range switch with OFF, ZERO, and BATT
checking positions.
Show controls on the
instrument
1) Switch ranges labeled as 5, 50, 500, and 5,000
2) ZERO position works in conjunction with ZERO
knob to electronically zero the meter.
NOTE: Mechanical
zero is adjusted using
screw on meter face
when the instrument is
off and should have
been adjusted at the last
calibration.
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3) BAT1 and BAT2 positions check the two batteries
used to power the instrument circuitry.
NOTE: The third
battery in the
instrument supplies the
detector bias, which is
minimal and does not
have a battery check
position.
4) OFF position turns the instrument off.
10. The effective center markings on the RO-2 are the
"dimples" or depressions on the sides and front of the
instrument case.
Show markings on the
instrument
11. Specific limitations/characteristics
a. The response time for the RO-2 series of instruments
is 5 seconds to reach 90% of the full value.
b. Geotropism, or the effect of gravity on the instrument,
causes no greater than a +2% of full scale change from
the actual value.
c. Correction factors may be needed when the radiation
field is not uniform over the entire detector.
d. High humidity or moisture can cause leakage currents
in the detector and cause erratic meter readings.
1) The detector is vented through a silica gel
desiccant, or drying medium, contained in a plastic
box.
2) The desiccant can become saturated and will need
replacement if the crystals start to turn clear or
pink instead of the normal blue color.
e. The detector is vented to atmosphere; therefore, any
change in atmospheric density changes the air density
in the detector.
1) An increase in temperature will lower the air
density in the detector and cause a lower response.
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2) An increase in atmospheric pressure will cause an
increase in air density in the detector and cause a
higher response.
3) Tables are provided in the technical manuals for
correcting the instrument response due to changes
in pressure or temperature.
4) A change in response of about 10% will occur if
the instrument was calibrated at room temperature
and used in an environment that is different by
about 50 �F.
f. Because the detector is vented to atmosphere,
radioactive gases can enter the detector and cause a
reading.
D. Bicron RSO-50 and RSO-500 Instruments
Section 6
1. The Bicron RSO-50 and RSO-500 instruments are
portable air-vented ion chamber instruments used to
detect and measure gamma, x-ray, and beta radiation.
Show instruments.
2. The Bicron RSO series of instruments are very similar in
design and construction to the Eberline RO-2 series of
instruments.
3. Detector (identical for both models)
a. Operated as an ionization chamber
b. A phenolic, or plastic, cylinder of 3 in. diameter and
12.7 in3 (208 cm3) volume with one end open but
covered by a Mylar window.
c. Fill gas - air (vented to atmosphere through a silica gel
desiccant pack)
4. The Bicron RSO series instruments are operated in the
current mode, or the mode that averages the individual
pulse heights per unit time.
5. The instrument ranges of the two models are as follows:
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a. RSO-500 Ranges:
0-0.5 R/hr
0-5 R/hr
0-50 R/hr
0-500 R/hr
b. RSO-50 Ranges:
0-50 mR/hr
0-500 mR/hr
0-5 R/hr
0-50 R/hr
6. The active volume of the detector is shielded from the
side by the detector wall and the instrument case and from
the bottom by the movable beta shield and two layers of
windows.
a. Detector wall is 200 mg/cm2 and the 0.13 cm
aluminum case is about 345 mg/cm2.
b. The materials and density-thickness value of the two
windows, one on the case and one on the detector, are
the same for both models.
Show instrument
windows.
1) RSO windows - 7 mg/cm2 total, both windows are
Mylar of 3.5 mg/cm2 each
c. The sliding beta shield is made of phenolic and the
density-thickness value is the same for both models.
Show instrument
sliding shield.
1) RSO shield - 400 mg/cm2 (1/8 in. thick) and is
mounted externally on the case
7. The Bicron RSO series of instruments are designed to
measure gamma, x-ray and beta radiation but will detect
(not measure) fast neutron radiation.
a. The instruments will read approximately 10%, in
mR/hr, of the true neutron field, in mrem/hr.
b. Like the Eberline RO-2, the Bicron RSO series
instruments will not respond to alpha radiation
because the alpha particles are shielded before they
reach the detector.
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8. The energy response of the two models is identical.
a. Both models measure photon radiation within +20%
for photon energies from 12 keV to 7 MeV (beta
shield open).
b. The minimum energy increases to 25 keV if the shield
is closed, and to about 40 keV through the side of the
instrument.
c. Both models measure beta radiation >70 keV.
9. Operator-adjustable controls
a. RSO-500 range switch with OFF, ZERO, and BATT
checking positions.
1) Switch ranges labeled as 0.5, 5, 50, and 500 R/hr
2) ZERO position works in conjunction with ZERO
knob to electronically zero the meter.
3) BAT position checks the two batteries used to
power the instrument circuitry and detector bias.
4) OFF position turns the instrument off.
b. RSO-50 range switch is the same but is labeled 50 and
500 mR/hr and 5 and 50 R/hr.
10. The effective center markings on both Bicron models are
the stamped circles with a plus sign in the circle and are
located on the sides and front of the instrument case.
Show markings on
instrument.
If the radiation field over the whole detector is not
uniform (e.g. from surface contamination, radiation
streaming, or from a small point source) the displayed
value may need to be corrected.
11. Specific limitations/characteristics
Section 7
a. The response time varies between the two models of
Bicron instruments available.
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1) RSO-500 - approximately 10 seconds from 0-90%
of the final reading.
2) RSO-50 - approximately 5 seconds from 0-90% of
the final reading.
b. Correction factors may be needed when the radiation
field is not uniform over the entire detector.
c. High humidity or moisture can cause leakage currents
in the detector and cause erratic meter readings.
1) The detector is vented through a desiccant, or
drying medium, contained in a plastic box.
2) The desiccant can become saturated and will need
replacement if the crystals start to turn clear or
pink.
d. Like the Eberline RO-2, the detector is vented to
atmosphere; therefore, any change in atmospheric
density changes the air density in the detector.
1) An increase in temperature will lower the air
density in the detector and cause a lower response.
2) An increase in atmospheric pressure will cause an
increase in air density in the detector and cause a
higher response.
3) Tables are provided in the technical manuals for
correcting the instrument response due to changes
in pressure or temperature.
4) A change in response of about 10% will occur if
the instrument was calibrated at room temperature
and used in an environment that is different by
about 50oF.
e. Because the detector is vented to atmosphere,
radioactive gases can enter the detector and cause a
reading.
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E. Victoreen Model 450B
1. The Victoreen 450B is a portable, general purpose, ion
chamber survey instrument which uses microprocessor
and LCD (liquid crystal display) technology.
Show instrument.
2. Detector
a. Operated as an ionization chamber
b. A Bakelite, or plastic, cylinder of 200 cm3 volume
with one end open but covered by a Mylar window
c. Fill gas - air (vented to atmosphere through a
desiccant pack)
d. The ion chamber detector is designed as tissue-
equivalent, allowing the instrument to accurately
access the exposure rate to human tissue.
3. The Victoreen 450B is operated in the current mode as are
most ion chambers.
4. Instrument operating range
a. Overall range is 0-50 R/hr.
b. The instrument is auto-ranging, or automatically
changes scales as required for the instrument reading,
and has the following scales:
1) 0-5 mR/hr
2) 0-50 mR/hr
3) 0-500 mR/hr
4) 0-5 R/hr
5) 0-50 R/hr
5. The active volume of the detector is shielded from the
side by the detector wall and the instrument case and from
the bottom by the movable beta shield and windows.
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a. Detector wall is 200 mg/cm2.
b. The sliding beta shield is made of Bakelite, which is a
type of plastic and the density-thickness value is
440 mg/cm2.
c. The two detector windows, one on the detector and
one on the case, are made of 1.7 mil Mylar for a total
of 3.4 mg/cm2.
6. The 450B instrument is designed to measure gamma, x-
ray, beta and alpha radiation but will detect (not measure)
fast neutron radiation.
a. The instruments will read approximately 10%, in
mR/hr, of the true neutron field, in mrem/hr.
7. Energy response
a. Photon energy response (+20%) is about 20 keV for
slide open, 40 keV for slide closed, and 50 keV from
the side.
Section 8
b. Beta energies >32 keV can be measured. Tech
manual states 100 keV; however, the minimum
possible energy is 32 keV.
c. The alpha response is limited to energies >4 MeV and
only if the detector to source distance is less than the
alpha range in air. Recall that a 4 MeV alpha travels
~2.5 cm in air.
8. Operator-adjustable controls
a. Only three external controls are available on the 450B:
the ON/OFF switch, the MODE switch, and the meter
light button.
b. The Mode switch is used during calibration and is not
enabled for operator use.
c. The ON/OFF switch turns the instrument on and off.
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1) The instrument is auto-ranging and will change the
bar graph, digital value, and scale markings as
appropriate for the exposure rate value.
2) The instrument has an "auto-zero" feature that
eliminates any need for an external zero control.
3) If the batteries are low, then the instrument will
display a LOW BAT message.
d. A button switch is provided in the handle for turning
the meter face light on and off.
9. The effective center markings on the 450B are the
painted-white depressions in the plastic case and are
located in the front and on the sides.
Show markings.
10. Specific limitations/characteristics
a. The response times to 90% of the final value for the
450B instrument are as follows, assuming that a step
increase or decrease in the rate does not cause a range
change:
NOTE: The response
times may be greater
for a step change from
background to a rate
value (e.g., background
to 4 mR/hr - 9.3 sec).
1) 0-5 mR/hr - 8 sec
2) 0-50 mR/hr - 5 sec
3) 0-500 mR/hr - 2 sec
4) 0-5 R/hr - 2 sec
5) 0-50 R/hr - 2 sec
b. Geotropism, or the effect of gravity on the instrument,
causes no greater than a +1% of full scale change from
the actual value.
c. Correction factors may be needed when the radiation
field is not uniform over the entire detector, such as
for surface contamination beta dose rates.
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d. High humidity or moisture could cause leakage
currents in the detector and cause erratic meter
readings.
1) The detector is vented through a desiccant, or
drying medium, contained in a plastic cylinder.
2) The desiccant could become saturated and will
need replacement if the crystals start to turn clear
or pink.
3) The atmospheric vent on the case has a rubber
bladder to allow for changes in temperature and
pressure but prevents the free flow of air into and
out of the detector casing.
4) The rubber bladder minimizes the effects of high
humidity environments and radioactive gases.
e. The detector is vented to atmosphere; therefore, any
change in atmospheric density changes the air density
in the detector.
1) An increase in temperature will lower the air
density in the detector and cause a lower response.
2) An increase in atmospheric pressure will cause an
increase in air density in the detector and cause a
higher response.
3) The value of the changes due to temperature and
pressure are similar to those of other air-vented
ion chambers.
F. Eberline Teletector Objective 2.16.03
1. The Eberline Teletector is an extendable, telescoping-rod
instrument designed with two Geiger-Mueller detectors
for the measurement of photon exposure rates and
detection of beta radiation.
Show instrument.
NOTE: Manufactured
in W. Germany and
distributed in U.S. by
Eberline
Section 9
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2. Detectors
a. Both detectors are sealed GM tubes with halogen-
quenched argon fill gas contained in an energy
compensating case.
1) Energy compensation is required in GM
detectors to reduce the over-response to low
energy photons.
b. The low range detector is the largest of the two
detectors and is located at the end of the detector
housing.
1) The low range detector is used for the three
lowest ranges on the instrument.
c. The high range detector is the small cylinder
located on the offset circuit board in the detector
housing.
1) The high range detector is used for the upper
two scales.
d. The GM detectors are very sensitive; however,
they lack the direct correlation to energy deposited
and are not as useful as ion chamber instruments
for assessing exposure or exposure rates.
3. The Teletector instrument is operated in the pulse
mode, or the mode that counts each individual pulse.
a. Since any ionization in a GM tube causes the same
large pulse, any radiation interaction in the
detector will be counted.
b. All the pulses are of the same large size regardless
of the energy or type of radiation; therefore, all
information on the type and energy of the radiation
is lost.
4. The instrument range is 0 - 1000 R/hr.
The analog Teletector has five operating ranges, each
with its own meter face. The three lower ranges
Detector window
Show window and
rubber cap.
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utilize the large GM detector and the two upper ranges
utilize the smaller GM detector.
a. 0-2 mR/hr
b. 0-50 mR/hr
c. 0-2 R/hr
d. 0-50 R/hr
e. 0-1000 R/hr
5. Detector shielding
a. The two detectors are shielded by layers of lead
and fiber to reduce the low-energy photon
response.
b. The low-range detector has a 30 mg/cm2 mica
window and a rubber cap to protect the window.
Mica is used on GM
detectors, because
Mylar would react with
the halogen quench gas.
6. The Eberline Teletector will measure x-ray and
gamma radiation and can detect (but not measure) beta
radiation.
a. Beta response is not accurate and should be used
for detection purposes only as stated in the
manufacturer's instructions.
b. Alpha response is eliminated by the thicker
window and casing.
c. Neutron response is insignificant due to the lower
probability of interaction in the small detectors.
7. Energy response
a. The energy response for photon radiation is 80
keV to 3 MeV (+10%). If the detector is not
pulled out of the telescoping rod housing, the
minimum photon energy will be higher.
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b. Beta particles >160 keV can be detected but not
measured.
8. Operator-adjustable controls
a. The only control is the range switch with OFF and
B (battery check) positions.
Show instrument.
b. Changing the range at the switch also changes the
rotating meter face to the appropriate meter face
for that range.
9. Detector effective center markings
a. The effective center of both detectors is indicated
by the machined grooves in the detector housing,
with the groove closest to the beta window
indicating the low-range detector.
b. The high range detector is mounted on a circuit
board and is not centered in the detector housing.
1) The offset is indicated by the machined groove
in the housing retaining ring at the back end of
the detector housing.
Section 10
2) Any contact readings taken using the high
range detector should align the offset indicator
so that it points to the source of radiation.
Failure to do so will result in inconsistent
readings.
10. Specific limitations/characteristics
a. Response time for the instrument is approximately
1 second to 90% of full scale.
b. The sealed detectors do not require correction
factors for temperature or pressure.
c. The sealed detectors do not experience problems
with humidity or radioactive gases entering the
detector.
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d. Since beta radiation is only detected and not
measured, no correction factors are applied for
beta radiation.
e. The 13 ft telescoping rod is durable but can be
damaged if twisted or bent.
f. Audible indication is available only through the
speaker jack; no internal speaker is installed.
g. The Eberline Teletector is non-saturating on the
high ranges up to 30,000 R/hr.
1) For GM detectors, the possibility exists that
the detectors become saturated in very high
radiation fields. Some GM detector
instruments will read zero if the detector
becomes saturated.
G. Eberline RO-7 Objective 2.16.03
1. The RO-7 series instrument provides remote monitoring
in high range beta and gamma radiation fields.
Show instrument.
a. The RO-7 consists of a basic digital readout
instrument, three interchangeable detectors, and
various interconnecting devices.
b. The detectors may be interconnected to the instrument
by flexible cables of different lengths, by rigid
extensions of different lengths or by use of an
underwater housing.
2. Detectors
a. All three detectors are air-vented ion chambers
contained in a plastic-lined (phenolic) aluminum
housing. The detector fill gas is air.
Show detectors.
b. The detector housing also contains other electronics,
such as an operational amplifier and detector
identification circuitry.
c. The three available detectors are as follows:
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1) The RO-7-LD is a low-range, gamma-only
detector with an active volume of about 50 cm3
and dimensions of 2.5 cm diameter and 10.2 cm
long.
2) The RO-7-BM is a mid-range, beta/gamma
detector, with beta window, that has an active
volume of about 7 cm3 and dimensions of 2.5 cm
diameter and 1.5 cm long.
3) The RO-7-BH is a high-range, beta/gamma
detector, with beta window, that has an active
volume of about 7 cm3 and dimensions of 2.5 cm
diameter and 1.5 cm long.
d. Each detector is labeled at the connector end of the
detector.
NOTE: Two small screws on the label are marked
ZERO and CAL. These should only be adjusted at
calibration and must not be adjusted by the operator.
3. The RO-7 instrument is operated in the current mode of
operation.
4. The operating range of the instrument is dependent on the
detector that is connected to the instrument.
a. The range of the RO-7-LD detector is 0-2 R/hr.
b. The range of the RO-7-BM detector is 0-200 R/hr.
c. The range of the RO-7-BH detector is 0-20 kR/hr
(20,000 R/hr).
5. Detector shielding
All three detectors have the phenolic liner and aluminum
housing.
Detector window
Show window.
a. The RO-7-BM and RO-7-BH detectors each have a 7
mg/cm2 Mylar window.
b. The Lucite cap for the beta window is 100 mg/cm2.
Show cap.
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Section 11
6. Types of radiation detected/measured
a. As previously mentioned, the RO-7-LD detector
measures only gamma and x-ray radiation.
1) Both beta and alpha radiation are shielded by the
detector housing.
2) Neutron radiation response is insignificant due to
the small size of the detector.
b. The actual detectors in the RO-7-BM and RO-7-BH
detector assemblies are identical.
1) Both detect and measure gamma, x-ray, and beta
radiation.
2) Alpha response is eliminated by the 7 mg/cm2
window (same density thickness as the dead layer
of skin).
3) Neutron radiation response is even smaller than
the RO-7-LD due to the smaller detector volume.
7. The energy response for the three detectors is as follows:
a. The RO-7-LD responds to photon radiation between
50 keV and 1.3 MeV (+20%).
b. The RO-7-BM and RO-7-BH detectors respond to
photon radiation differently depending on orientation
and whether the Lucite cover is in place.
1) Lucite cover off - 10 keV to 1.3 MeV (+20%)
2) Lucite over on - 25 keV to 1.3 MeV (+20%)
3) Shield on, from the side - 50 keV to 1.3 MeV
(+20%)
c. The beta response for the RO-7-BM and RO-7-BH
detectors is for beta energies >70 keV.
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8. Operator-adjustable controls
a. The ON/OFF switch is the only range control because
the instrument identifies the detector model and
adjusts the readout accordingly.
1) A low battery condition is indicated by a "colon"
under the battery mark on the meter.
b. The ZERO knob will zero the LCD readout.
c. A meter face light is turned on/off by the small switch
in front of the pistol grip.
9. No markings are provided for the detector effective
center.
10. Specific limitations/characteristics
a. The response time of the basic instrument is 2.5
seconds to 90% of the final reading.
b. The correction factor for the true beta measurement is
1.5 as recommended by the manufacturer.
c. Since the detector is air-vented, atmospheric
temperature and pressure changes affect the
instrument reading.
1) The instrument response will remain within +10%
for the temperature range of -20 to 160 �F.
2) A correction table is available in the technical
manual for pressure changes.
d. The detectors are air-vented but do not have a
desiccant pack. The detector should be kept dry and
out of high humidity environments to prevent leakage
currents.
e. Each detector has associated electronics designed for
that particular range. Over-ranging a detector may
cause damage to the detector electronics.
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f. If the instrument is not calibrated with the underwater
housing and the housing is used, the response will be
about 5% low. The instrument reading should be
multiplied by 1.05 to obtain the corrected response.
g. Interconnecting devices from the detector to the
instrument that are available from the manufacturer
are the:
1) 15 ft flexible cable
2) 60 ft flexible cable
3) 2 ft rigid extension
4) 5 ft rigid extension
5) Stainless-steel underwater housing with 60 ft of
cable
H. Eberline NRD Neutron Sphere Objective 2.16.04
1. The Eberline NRD sphere is a portable instrument for the
detection and measurement of the dose equivalent rate
from neutron radiation.
Show instrument.
2. Detector
a. The detector is the Eberline NRD (neutron radiation
detector) sphere, which may be connected to the PNR-
4 or to an ESP instrument by a coaxial cable.
Section 12
Show detector.
b. The NRD sphere is a 9 in. diameter, cadmium loaded,
polyethylene sphere with a BF3 proportional tube in
the center of the sphere.
c. The BF3 (boron trifluoride) detector design allows the
detection of only thermal neutrons because of the low
probability of absorption by boron for other energy
neutrons.
Recall thermal neutrons
are defined as those
neutrons with kinetic
energy in thermal
equilibrium with their
surroundings, or 0.025
eV at STP.
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1) The thermal neutron capture reaction with the 10B
results in gas ionization pulses caused by the alpha
particle product of the reaction.
A less prominent
reaction is:
10
5B (N,2α) 3
1He
1
0n + 10
5B � 7
3Li + 42He
or
10
5B (n,α) 73Li
2) Detector shielding must be employed if the
detector is used for measurement of neutron
energies other than thermal.
3. Detector shielding (no window)
a. A polyethylene sphere is used to allow assessment of
the dose equivalent from fast and intermediate energy
neutrons.
1) The polyethylene has a high percentage of
hydrogen which thermalizes the fast and
intermediate energy neutrons.
2) Those neutrons that are thermalized in the sphere
can be detected in the BF3 tube.
3) The diameter of the sphere is chosen during design
for the neutron energy spectrum expected to be
measured.
b. The cadmium loading is a thin, perforated sheet of
cadmium surrounding the active volume of the
detector and is designed to reduce the over-response
of the detector to certain energy neutrons. May over-
respond by 100-300% for intermediate neutrons
without Cd shield.
4. Operating range
a. The PNR-4 has an overall range of 0-5,000 mrem/hr.
b. PNR-4 has a LIN-LOG meter which means the meter
face is a combination of linear and logarithmic scales.
1) The auto-ranging meter uses two meter needles
and covers four decades (logarithmic portion).
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2) Within each decade of the range, the meter
divisions are equally spaced (linear portion).
3) The first needle covers the first two decades of 0-5
mrem/hr and 5-50 mrem/hr.
4) The second needle covers the last two decades of
50-500 mrem/hr and 500-5,000 mrem/hr.
5. Types of radiation detected and measured
a. The instrument is designed for detection and
measurement of fast and intermediate energy neutron
radiation.
b. Alpha and beta radiation are not detected because they
do not penetrate the detector shielding.
c. Gamma radiation passes through the detector
shielding but can be rejected by the instrument
circuitry up to 500 R/hr (dependent on high voltage
setting and desired rejection level). At low rates,
photon pulses are rejected. At high rates, pulse pile-
up causes a gamma response.
d. Since the detector is operated in the proportional
region, the pulses from the alpha particles are larger
than pulses from other interactions and trigger a pulse
height discriminator in the instrument circuitry.
e. The mode of operation for the instrument is the pulse
mode so that individual pulses can be discriminated
and counted.
6. Energy response for measured radiation
a. The instrument manufacturer states the instrument
response closely follows the theoretical dose
equivalent from neutrons over a range of 0.025 eV to
about 10 MeV.
b. The instrument over-responds to intermediate energy
neutrons and under-responds to relativistic neutrons.
Section 13
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7. Operator-adjustable controls
a. The only operator-adjustable control on the PNR4 is
the OFF/ON/BAT switch which turns the instrument
on and off and allows a check of the battery.
8. Specific limitations/characteristics
a. The response time depends on which decade of the
scale is appropriate.
1) First decade - 12 seconds
2) Second decade - 6 seconds
3) Third decade - 1.5 seconds
4) Fourth decade - 0.3 seconds
b. No correction factors are necessary.
c. The detector is a sealed pressurized cylinder and is not
affected by changes in humidity, radioactive gases or
changes in atmospheric density.
I. Eberline ASP-1 with NRD Sphere
1. The Eberline ASP-1 with the NRD sphere is a
microcomputer-based, analog-display, portable neutron
radiation survey instrument.
Show instrument.
2. The detector (Eberline NRD sphere) is identical to the
detector used with the PNR-4 neutron instrument.
3. The mode of operation is the pulse mode.
4. Instrument operating ranges NOTE: The operating
ranges are established
by the calibrating
facility based on the
detector used and
intended purpose by
using interchangeable
switch labels.
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a. The overall range is 0-100 rem/hr and has a useable
range of 1 mrem/hr - 60 rem/hr per HP procedure.
1) 0-1 mrem/hr
2) 0-10 mrem/hr
3) 0-100 mrem/hr
4) 0-1,000 mrem/hr
5) 0-10,000 mrem/hr
6) 0-100,000 mrem/hr
5. Detector shielding is the same as previously mentioned
for the NRD sphere.
6. The energy response is the same as previously mentioned
for the NRD sphere.
7. Operator-adjustable controls
a. The OFF/BAT/HV/range switch has the following
functions:
1) The OFF position turns the instrument off.
2) The BAT position checks the instrument battery
power supply.
3) The HV position checks the applied high voltage
to the detector and should match the value listed
on the special label on the instrument case.
4) The range markings are X1, X10, X100, X1K,
X10K, and X100K with a meter scale of 0-1.0.
b. The INTEGRATE/FAST/SLOW switch is a three
position toggle switch with the following functions:
1) In the INTEGRATE position, the instrument will
show the total dose equivalent accumulated since
the last time the instrument was reset to zero or
turned off.
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2) In the FAST position, the response time selected
by the microcomputer is for typical survey work.
3) In the SLOW position, the response is slower but
with greater accuracy than the FAST position.
c. The LIGHT/RESET switch is a three-position, spring-
loaded toggle switch with the following functions:
1) The LIGHT position illuminates the meter face.
2) The RESET position will zero the meter reading
for the current
mode (INTEGRATE/FAST/SLOW) setting of the
instrument.
3) The RESET switch will cause the "standard
current" value to be displayed if held for 5 seconds
while in the FAST or SLOW mode.
This is utilized as a
calibration check when
compared to
predetermined value.
d. The SPEAKER is a two-position toggle switch for
turning the external speaker on and off.
e. Acoustic (airline-type) head phones can be plugged
into the speaker cover on the top of the instrument.
8. As previously mentioned, the NRD sphere has no
effective center markings.
9. Specific limitations/characteristics
Section 14
a. The response time of the instrument is controlled by
the microcomputer and is based on the input count
rate and whether the mode switch is in FAST or
SLOW.
1) In the FAST position, the instrument response
time varies between one and ten seconds.
2) In the SLOW position, the instrument response
time will vary up to a maximum of 29 seconds.
b. No correction factors are required to correct the
displayed value.
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c. The sealed detector is not affected by changes in
atmospheric density, humidity or radioactive gases.
d. The instrument has a microcomputer controlled "over-
range" indication.
1) When the radiation rate exceeds the useful range
of the detector, the computer will cause an over-
range alarm.
2) When the instrument alarms, the meter needle will
sweep back and forth and an interrupted tone will
sweep in the speaker.
J. Portable Instrument Specification Chart
1. The specifications for the instruments discussed can be
summarized in a chart that shows:
a. manufacturer
b. model
c. detector type
d. operating ranges
e. detector shield
f. detector window
g. radiation measured
h. radiation detected (but not measured)
i. response times.
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III. SUMMARY
A. Review major points
1. General discussion
2. Factors affecting instrument selection
3. Eberline RO-2 series
4. Bicron RSO-50 and RSO-500
5. Victoreen 450B
6. Eberline Teletector
7. Eberline RO-7
8. Eberline PNR-4 with NRD sphere
9. Eberline ASP-1 with NRD sphere
B. Review learning objectives
IV. EVALUATION
Evaluation should consist of a written examination comprised of
multiple choice, fill-in the blank, matching and/or short answer
questions. 80% should be the minimum passing criteria for
examinations.
Module Number: 2.16