Radiographic Testing Compiled for ASNT by Bahman Zoofan The Ohio State University
Radiographic TestingRadiographic Testing
Compiled for ASNT byBahman Zoofan
The Ohio State University
Compiled for ASNT byBahman Zoofan
The Ohio State University
Level I
Radiographic Testing
Level I
Radiographic Testing
Lesson 1Lesson 1
Introduction to Radiographic Testing
Introduction to Radiographic Testing
RadiographyRadiography
1. In radiography, test objects are
exposed to X-rays, gamma rays
or neutrons, and an image is
processed.
1. In radiography, test objects are
exposed to X-rays, gamma rays
or neutrons, and an image is
processed.
RadiographyRadiography
2. Radiography is used to test a variety of
products, such as castings, forgings
and weldments. It is also used heavily
in the aerospace industry for the
detection of cracks in airframes
structures, detection of water in
honeycomb structures and for foreign
object detection.
2. Radiography is used to test a variety of
products, such as castings, forgings
and weldments. It is also used heavily
in the aerospace industry for the
detection of cracks in airframes
structures, detection of water in
honeycomb structures and for foreign
object detection.
Advantages of Radiographic TestingAdvantages of Radiographic Testing
1. Radiography can be used on most materials.
2. Radiography provides a permanent record of the test object.
3. Radiography reveals discontinuities within a material.
4. Radiography discloses fabrication errors and often indicates the need for corrective action.
1. Radiography can be used on most materials.
2. Radiography provides a permanent record of the test object.
3. Radiography reveals discontinuities within a material.
4. Radiography discloses fabrication errors and often indicates the need for corrective action.
Limitations of Radiographic TestingLimitations of Radiographic Testing
1. The radiographer must have access to both sides of the test object.
2. Planar discontinuities that are not parallel to the radiation beam are difficult to detect.
1. The radiographer must have access to both sides of the test object.
2. Planar discontinuities that are not parallel to the radiation beam are difficult to detect.
Limitations of Radiographic TestingLimitations of Radiographic Testing
3. Radiography is an expensive testing method.
4. Film radiography is time consuming.
5. Some surface discontinuities or shallow discontinuities may be difficult, if not impossible, to detect.
3. Radiography is an expensive testing method.
4. Film radiography is time consuming.
5. Some surface discontinuities or shallow discontinuities may be difficult, if not impossible, to detect.
Test ObjectiveTest Objective
The objective of radiographic testing is to
ensure product reliability. Performing the
actual radiographic test is only part of the
procedure. The results of the test must
then be interpreted to acceptance
standards by qualified personnel, and an
evaluation of the results must be made.
The objective of radiographic testing is to
ensure product reliability. Performing the
actual radiographic test is only part of the
procedure. The results of the test must
then be interpreted to acceptance
standards by qualified personnel, and an
evaluation of the results must be made.
Safety ConsiderationsSafety Considerations
Radiation can cause damage to the
cells of living tissue, so it is essential
that personnel be aware and
protected. Compliance with state and
federal safety regulations is
mandatory.
Radiation can cause damage to the
cells of living tissue, so it is essential
that personnel be aware and
protected. Compliance with state and
federal safety regulations is
mandatory.
QualificationQualification
1. It is important that personnel
responsible for radiographic testing
have adequate training, education
and experience.
2. Guidelines are for the qualification
and certification of nondestructive
testing personnel.
1. It is important that personnel
responsible for radiographic testing
have adequate training, education
and experience.
2. Guidelines are for the qualification
and certification of nondestructive
testing personnel.
QualificationQualification
3. ASNT has published guidelines for training and qualifying nondestructive testing (NDT) personnel since 1966. These are known as: Personnel Qualification and Certification in Nondestructive Testing: Recommended Practice No. SNT-TC-1A.
3. ASNT has published guidelines for training and qualifying nondestructive testing (NDT) personnel since 1966. These are known as: Personnel Qualification and Certification in Nondestructive Testing: Recommended Practice No. SNT-TC-1A.
QualificationQualification
4. Recommended Practice No.
SNT-TC-1A describes the
knowledge and capabilities of
nondestructive testing personnel
in terms of certification levels.
4. Recommended Practice No.
SNT-TC-1A describes the
knowledge and capabilities of
nondestructive testing personnel
in terms of certification levels.
QualificationQualification
5. Per SNT-TC-1A, there are three
basic levels of qualification applied
to nondestructive testing personnel:
a. Level I.
b. Level II.
c. Level III.
5. Per SNT-TC-1A, there are three
basic levels of qualification applied
to nondestructive testing personnel:
a. Level I.
b. Level II.
c. Level III.
CertificationCertification
1. The formal certification of a person in nondestructive testing to a Level I, Level II and Level III is a written testimony that the individual has been properly qualified.
2. Certification is meant to document the actual qualification of the individual in a specific nondestructive testing method.
1. The formal certification of a person in nondestructive testing to a Level I, Level II and Level III is a written testimony that the individual has been properly qualified.
2. Certification is meant to document the actual qualification of the individual in a specific nondestructive testing method.
CertificationCertification
3. Proper qualification and
certification is extremely
important in modern
manufacturing, fabrication and
inservice inspection due to the
impact on the health and safety
of the public.
3. Proper qualification and
certification is extremely
important in modern
manufacturing, fabrication and
inservice inspection due to the
impact on the health and safety
of the public.
Lesson 2Lesson 2
Radiographic Testing PrinciplesRadiographic Testing Principles
Penetration and Differential Absorption
Penetration and Differential Absorption1. X-rays and gamma rays have the ability
to penetrate materials, including materials that do not transmit light.
2. Depending on the thickness and density of the material, and the intensity of the source being used, the amount of radiation that is transmitted through the test object will vary.
1. X-rays and gamma rays have the ability to penetrate materials, including materials that do not transmit light.
2. Depending on the thickness and density of the material, and the intensity of the source being used, the amount of radiation that is transmitted through the test object will vary.
Penetration and Differential Absorption
Penetration and Differential Absorption
3. The radiation transmitted through
the test object produces the
radiographic image.
3. The radiation transmitted through
the test object produces the
radiographic image.
Penetration and Differential Absorption
Penetration and Differential Absorption
The following figure illustrates the
partial absorption characteristics of
radiation. Thicker portions of the test
object or dense inclusions will appear
lighter because of more absorption of
the radiation.
The following figure illustrates the
partial absorption characteristics of
radiation. Thicker portions of the test
object or dense inclusions will appear
lighter because of more absorption of
the radiation.
Geometric Exposure PrinciplesGeometric Exposure Principles
1. A radiograph is a shadow picture of a
test object placed between the
film/detector and the X-ray or gamma
radiation source.
2. If the film/detector is placed too far
from the test object, the image will be
enlarged.
1. A radiograph is a shadow picture of a
test object placed between the
film/detector and the X-ray or gamma
radiation source.
2. If the film/detector is placed too far
from the test object, the image will be
enlarged.
Geometric Exposure PrinciplesGeometric Exposure Principles
3. If the test object is too close to the
source, the image will be greatly
enlarged, resulting in the loss of
resolution.
4. The degree of enlargement will
vary according to the relative
distances of the test object from the
film/detector.
3. If the test object is too close to the
source, the image will be greatly
enlarged, resulting in the loss of
resolution.
4. The degree of enlargement will
vary according to the relative
distances of the test object from the
film/detector.
Geometric Exposure PrinciplesGeometric Exposure Principles
5. As shown in the following figure,
the image enlargement: Df/D0 is
equal to the ratio: df/d0.
5. As shown in the following figure,
the image enlargement: Df/D0 is
equal to the ratio: df/d0.
Film/Detector Image SharpnessFilm/Detector Image Sharpness
1. The sharpness of a radiographic
image is determined by:
a. The size of the radiation
source.
b. The ratio of the object-to-film/
detector distance.
c. Source-to-object distance.
1. The sharpness of a radiographic
image is determined by:
a. The size of the radiation
source.
b. The ratio of the object-to-film/
detector distance.
c. Source-to-object distance.
Film/Detector Image SharpnessFilm/Detector Image Sharpness
2. The unsharpness or fuzziness
around an image is called geometric
unsharpness (penumbra), as shown
in the following figure.
2. The unsharpness or fuzziness
around an image is called geometric
unsharpness (penumbra), as shown
in the following figure.
Film/Detector Image SharpnessFilm/Detector Image Sharpness
3. To minimize the geometric unsharpness (Ug) in the image, the
test object should placed as close to the film/detector as possible.
4. Most radiographic codes recommend the maximum acceptable values for geometric unsharpness.
3. To minimize the geometric unsharpness (Ug) in the image, the
test object should placed as close to the film/detector as possible.
4. Most radiographic codes recommend the maximum acceptable values for geometric unsharpness.
Film/Detector Image SharpnessFilm/Detector Image Sharpness
5. Geometric unsharpness can be
calculated using the following
formula:
Ug = Fd/D
5. Geometric unsharpness can be
calculated using the following
formula:
Ug = Fd/D
Film/Detector Image SharpnessFilm/Detector Image Sharpness
a. Ug is the geometric unsharpness (in
millimeters or inches).
b. F is the source size (the maximum
projected dimension of the radiation
source, or effective focal spot size).
a. Ug is the geometric unsharpness (in
millimeters or inches).
b. F is the source size (the maximum
projected dimension of the radiation
source, or effective focal spot size).
Film/Detector Image SharpnessFilm/Detector Image Sharpness
c. D is the distance from the source
of the radiation to the object
being radiographed.
d. d is the distance from the source
side of the test object to the
film/detector.
c. D is the distance from the source
of the radiation to the object
being radiographed.
d. d is the distance from the source
side of the test object to the
film/detector.
Film/Detector Image SharpnessFilm/Detector Image Sharpness
5. Optimum geometric unsharpness of
the image is obtained when:
a. The radiation source is small.
b. The distance from the source to
the test object is relatively large.
c. The distance from the test object
to the film/detector plane is small.
5. Optimum geometric unsharpness of
the image is obtained when:
a. The radiation source is small.
b. The distance from the source to
the test object is relatively large.
c. The distance from the test object
to the film/detector plane is small.
Image DistortionImage Distortion
Two possible causes of radiographic
image distortion are:
1. The test object and the film/
detector plane are not parallel.
2. The radiation beam is not directed
perpendicular to the film/detector
plane.
Two possible causes of radiographic
image distortion are:
1. The test object and the film/
detector plane are not parallel.
2. The radiation beam is not directed
perpendicular to the film/detector
plane.
X-Radiation and Gamma RadiationX-Radiation and Gamma Radiation
1. X-rays and gamma rays are part
of the electromagnetic spectrum.
2. They have high energy and short
wavelengths.
1. X-rays and gamma rays are part
of the electromagnetic spectrum.
2. They have high energy and short
wavelengths.
X-RaysX-Rays
The conditions required to generate
X-rays are:
1. A source of electrons.
2. A suitable target for electrons to
strike.
3. A means of speeding the electrons
in the desired direction.
The conditions required to generate
X-rays are:
1. A source of electrons.
2. A suitable target for electrons to
strike.
3. A means of speeding the electrons
in the desired direction.
X-RaysX-Rays
Characteristic X-rays: When an
electron of sufficient energy
interacts with an orbital electron
of an atom, then characteristic
X-rays may be generated.
Characteristic X-rays: When an
electron of sufficient energy
interacts with an orbital electron
of an atom, then characteristic
X-rays may be generated.
X-RaysX-Rays
Continuous radiation: The
generated X-rays have a continuous
energy spectrum and not entirely
dependent on the disturbed atoms
characteristics.
Continuous radiation: The
generated X-rays have a continuous
energy spectrum and not entirely
dependent on the disturbed atoms
characteristics.
X-RaysX-Rays
Bremsstrahlung radiation: This is a
German name for braking or
continuous radiation.
Bremsstrahlung radiation: This is a
German name for braking or
continuous radiation.
X-RaysX-Rays
KeV (kilo-electron volts): The
unit corresponds to the amount
of kinetic energy that an electron
would gain when moving
between two points that differ in
voltage by 1 kV.
KeV (kilo-electron volts): The
unit corresponds to the amount
of kinetic energy that an electron
would gain when moving
between two points that differ in
voltage by 1 kV.
X-RaysX-Rays
MeV (1000,000 electron volts): This
unit corresponds to the amount of
kinetic energy of electrons when
moving between two points that
different by 1MV.
MeV (1000,000 electron volts): This
unit corresponds to the amount of
kinetic energy of electrons when
moving between two points that
different by 1MV.
Electron SourceElectron Source
1. When a suitable material is heated,
some of its charged negative particles
(electrons) become agitated and
escape the material as free electrons.
2. Cathode: In an X-ray tube, a coil of
wire (filament) is the source of
electrons (known as the cathode).
1. When a suitable material is heated,
some of its charged negative particles
(electrons) become agitated and
escape the material as free electrons.
2. Cathode: In an X-ray tube, a coil of
wire (filament) is the source of
electrons (known as the cathode).
Electron TargetElectron Target
For industrial radiography
application, a solid material of
high atomic number, usually
tungsten, is used as the target in
the tube anode.
For industrial radiography
application, a solid material of
high atomic number, usually
tungsten, is used as the target in
the tube anode.
Electron AccelerationElectron Acceleration
1. By placing a positive charge on
the anode of an X-ray tube and a
negative charge on the cathode,
free electrons are accelerated
from the cathode to the anode.
2. The electron path should be in a
vacuum.
1. By placing a positive charge on
the anode of an X-ray tube and a
negative charge on the cathode,
free electrons are accelerated
from the cathode to the anode.
2. The electron path should be in a
vacuum.
Radiation IntensityRadiation Intensity
1. The number of X-rays created
by electrons striking the
target is one measure of the
intensity of the X-ray beam.
2. Intensity depends on the
amount of electrons available
at the X-ray tube cathode.
1. The number of X-rays created
by electrons striking the
target is one measure of the
intensity of the X-ray beam.
2. Intensity depends on the
amount of electrons available
at the X-ray tube cathode.
Radiation IntensityRadiation Intensity
3. Keeping the other factors constant,
an increase in the current through
the tube filament will increase the
cathode temperature, causing
emission of more electrons and
consequently increasing the intensity
of the X-ray beam.
3. Keeping the other factors constant,
an increase in the current through
the tube filament will increase the
cathode temperature, causing
emission of more electrons and
consequently increasing the intensity
of the X-ray beam.
Radiation IntensityRadiation Intensity
4. Similarly, though to a lesser
degree, an increase in the applied
tube voltage will increase the
beam intensity.
5. The output rating of an X-ray tube
is expressed in volts (kV or MeV).
4. Similarly, though to a lesser
degree, an increase in the applied
tube voltage will increase the
beam intensity.
5. The output rating of an X-ray tube
is expressed in volts (kV or MeV).
Inverse Square LawInverse Square Law
1. The intensity of an X-ray beam varies inversely with the square of the distance from the radiation source.
I1/I2 = D22/D2
1
2. The relationship is known as the inverse square law: where I1 and I2 are the received radiation intensities at distances D1 and D2.
1. The intensity of an X-ray beam varies inversely with the square of the distance from the radiation source.
I1/I2 = D22/D2
1
2. The relationship is known as the inverse square law: where I1 and I2 are the received radiation intensities at distances D1 and D2.
X-Ray Quality CharacteristicsX-Ray Quality Characteristics
1. The spectrum of continuous X-rays
covers a wide band of wavelengths,
as shown in the following figure.
1. The spectrum of continuous X-rays
covers a wide band of wavelengths,
as shown in the following figure.
X-Ray Quality CharacteristicsX-Ray Quality Characteristics
2. An increase in applied voltage in an X-
ray tube increases the intensity (quality
of X-rays). This produces the generation
of the higher energy rays with greater
penetrating power.
3. X-rays with higher energy (shorter
wavelengths) are called hard
X-rays.
2. An increase in applied voltage in an X-
ray tube increases the intensity (quality
of X-rays). This produces the generation
of the higher energy rays with greater
penetrating power.
3. X-rays with higher energy (shorter
wavelengths) are called hard
X-rays.
X-Ray Quality CharacteristicsX-Ray Quality Characteristics
4. X-rays with lower energy (longer
wavelengths) are called soft X-rays.
5. Variation in tube current varies the
intensity of the beam, but the
spectrum of wavelengths produced
remains unchanged, as seen in the
following figure.
4. X-rays with lower energy (longer
wavelengths) are called soft X-rays.
5. Variation in tube current varies the
intensity of the beam, but the
spectrum of wavelengths produced
remains unchanged, as seen in the
following figure.
X-Ray Quality CharacteristicsX-Ray Quality Characteristics
6. Effects of changes in kilovoltage
and tube current on the produced
X-rays are summarized in
the following table.
6. Effects of changes in kilovoltage
and tube current on the produced
X-rays are summarized in
the following table.
Effects of kilovoltage and amperageEffects of kilovoltage and amperage
Interaction With MatterInteraction With Matter
1. Any action that disrupts the
electrical balance of an atom and
produces ions is called
ionization.
2. X-rays passing through matter
cause ionization in their path.
1. Any action that disrupts the
electrical balance of an atom and
produces ions is called
ionization.
2. X-rays passing through matter
cause ionization in their path.
Interaction With MatterInteraction With Matter
3. X-rays are photons (bundles of energy) traveling at the speed of light.
4. In passing through matter, X-rays lose energy to atoms by ionization processes knows as:
a. Photoelectric absorption.
b. Compton effect.
c. Pair production.
3. X-rays are photons (bundles of energy) traveling at the speed of light.
4. In passing through matter, X-rays lose energy to atoms by ionization processes knows as:
a. Photoelectric absorption.
b. Compton effect.
c. Pair production.
Photoelectric AbsorptionPhotoelectric Absorption
1. In photoelectric absorption, when
X-rays (photons) with relatively low
energy pass through matter, the
photon energy may be transferred to
an orbital electron (see the following
figure).
1. In photoelectric absorption, when
X-rays (photons) with relatively low
energy pass through matter, the
photon energy may be transferred to
an orbital electron (see the following
figure).
Photoelectric AbsorptionPhotoelectric Absorption
2. Part of the energy is expended in
ejecting the electron from its orbit,
and the remainder gives velocity to
the electron.
2. Part of the energy is expended in
ejecting the electron from its orbit,
and the remainder gives velocity to
the electron.
Photoelectric AbsorptionPhotoelectric Absorption
3. This phenomenon usually takes
place with low energy photons
of 0.5 MeV or less.
4. It is this absorption effect that
makes radiography possible.
3. This phenomenon usually takes
place with low energy photons
of 0.5 MeV or less.
4. It is this absorption effect that
makes radiography possible.
Compton EffectCompton Effect
1. When higher energy photons (0.1 to 3 MeV) pass through matter, part of the photon energy is expended in ejecting an electron. The remaining slower energy photons travel at different angles compared to the original photon path (see the following figure).
1. When higher energy photons (0.1 to 3 MeV) pass through matter, part of the photon energy is expended in ejecting an electron. The remaining slower energy photons travel at different angles compared to the original photon path (see the following figure).
Compton EffectCompton Effect
2. This process, progressively
weakening the photon, is
repeated until the photoelectric
effect completely absorbs the
last photon.
2. This process, progressively
weakening the photon, is
repeated until the photoelectric
effect completely absorbs the
last photon.
Pair ProductionPair Production
Pair production occurs only with
higher energy photons of 1.02 MeV
or more (see the following figure).
Pair production occurs only with
higher energy photons of 1.02 MeV
or more (see the following figure).
Scatter RadiationScatter Radiation
1. The major components of scatter
radiation are the low energy rays
represented by photons weakened
in the compton process.
2. Scatter radiation is low-level energy
content and of random direction.
1. The major components of scatter
radiation are the low energy rays
represented by photons weakened
in the compton process.
2. Scatter radiation is low-level energy
content and of random direction.
Internal ScatterInternal Scatter
1. Internal scatter is the scattering that
occurs in the object being
radiographed (see the following
figure).
1. Internal scatter is the scattering that
occurs in the object being
radiographed (see the following
figure).
Internal ScatterInternal Scatter
2. It affects image definition by
blurring the image outline.
3. The increase in radiation
passing through matter caused
by scatter in the forward
direction is known as buildup.
2. It affects image definition by
blurring the image outline.
3. The increase in radiation
passing through matter caused
by scatter in the forward
direction is known as buildup.
SidescatterSidescatter
1. Sidescatter is the scattering from
walls and the surrounding of the
object in the vicinity of the test
object that cause rays to enter the
sides of the test object.
2. Sidescatter obscures the image
outline just as internal scatter does.
1. Sidescatter is the scattering from
walls and the surrounding of the
object in the vicinity of the test
object that cause rays to enter the
sides of the test object.
2. Sidescatter obscures the image
outline just as internal scatter does.
Backscatter Backscatter
1. Backscatter is the scattering of
rays from the surface or from
objects beneath or behind the test
object (see the following figure).
2. Backscatter also obscures the
test object.
1. Backscatter is the scattering of
rays from the surface or from
objects beneath or behind the test
object (see the following figure).
2. Backscatter also obscures the
test object.
Gamma RaysGamma Rays
1. Gamma rays are produced by
the disintegration of the nuclei of
a radioactive isotope.
2. Isotopes are varieties of the
same chemical element having
different atomic weights.
1. Gamma rays are produced by
the disintegration of the nuclei of
a radioactive isotope.
2. Isotopes are varieties of the
same chemical element having
different atomic weights.
Gamma RaysGamma Rays
3. The wavelength and intensity of
gamma waves are determined by
the source isotope characteristics
and cannot be controlled or
changed.
3. The wavelength and intensity of
gamma waves are determined by
the source isotope characteristics
and cannot be controlled or
changed.
Natural Isotope SourcesNatural Isotope Sources
1. Some heavy natural elements
disintegrate because of their
inherent instability.
2. Radium is the best known and
most used natural radioactive
source.
1. Some heavy natural elements
disintegrate because of their
inherent instability.
2. Radium is the best known and
most used natural radioactive
source.
Natural Isotope SourcesNatural Isotope Sources
3. Natural radioactive sources release energy in the form of:
a. Gamma rays.
b. Alpha particles: Positively charged particles having mass and charge equal in magnitude of a helium nuclei.
c. Beta particles: Negatively charged particles having charge and mass as of the electron.
3. Natural radioactive sources release energy in the form of:
a. Gamma rays.
b. Alpha particles: Positively charged particles having mass and charge equal in magnitude of a helium nuclei.
c. Beta particles: Negatively charged particles having charge and mass as of the electron.
Natural Isotope SourcesNatural Isotope Sources
4. The penetrating power of alpha
and beta particles is relatively
negligible.
4. The penetrating power of alpha
and beta particles is relatively
negligible.
Artificial SourcesArtificial Sources
1. There are two ways of manufacturing
radioactive isotopes, or so-called
radioisotopes:
a. By using the by product of
nuclear fission in atomic
reactors, like cesium-137 (Cs-137).
1. There are two ways of manufacturing
radioactive isotopes, or so-called
radioisotopes:
a. By using the by product of
nuclear fission in atomic
reactors, like cesium-137 (Cs-137).
Artificial SourcesArtificial Sources
b. By bombarding certain elements
with neutrons to make them
unstable. Examples are:
cobalt-60 (Co-60), thulium-170
(Tm-170), selenium-75 (Se-75)
and iridium-192 (Ir-192).
2. These artificial isotopes emit gamma
rays, and alpha and beta particles.
b. By bombarding certain elements
with neutrons to make them
unstable. Examples are:
cobalt-60 (Co-60), thulium-170
(Tm-170), selenium-75 (Se-75)
and iridium-192 (Ir-192).
2. These artificial isotopes emit gamma
rays, and alpha and beta particles.
Gamma Ray IntensityGamma Ray Intensity
1. The activity of a gamma ray
source determines the intensity
of its radiation.
2. The measure of activity is the
curie (Becquerel) which is
3.7 X 1010 disintegrations per
second.
1. The activity of a gamma ray
source determines the intensity
of its radiation.
2. The measure of activity is the
curie (Becquerel) which is
3.7 X 1010 disintegrations per
second.
Specific ActivitySpecific Activity
1. Specific activity is defined as the
degree of concentration of
radioactive material within a
gamma ray source.
2. Specific activity is expressed in
terms of curies per gram or curies
per cubic centimeter.
1. Specific activity is defined as the
degree of concentration of
radioactive material within a
gamma ray source.
2. Specific activity is expressed in
terms of curies per gram or curies
per cubic centimeter.
Specific ActivitySpecific Activity
3. Specific activity is an important
measure of radioisotopes
because the smaller the source,
the sharper the radiographic
image that can be produced (as
shown in the following figure).
3. Specific activity is an important
measure of radioisotopes
because the smaller the source,
the sharper the radiographic
image that can be produced (as
shown in the following figure).
Half LifeHalf Life
1. The length of time required for the
activity of a radioisotope to decay to
one half of its initial intensity is
called its half life.
2. The half life of a radioisotope is a
basic characteristic, and depends
on the particular isotope of a given
element.
1. The length of time required for the
activity of a radioisotope to decay to
one half of its initial intensity is
called its half life.
2. The half life of a radioisotope is a
basic characteristic, and depends
on the particular isotope of a given
element.
Half LifeHalf Life
3. Dated decay curves (similar to one
shown in the next slide) are supplied
by source suppliers for each
particular radioisotope and should be
used by radiographers to determine
the exact source intensity.
3. Dated decay curves (similar to one
shown in the next slide) are supplied
by source suppliers for each
particular radioisotope and should be
used by radiographers to determine
the exact source intensity.
Gamma Ray Quality CharacteristicsGamma Ray Quality Characteristics
1. Radiation from a gamma ray source
consists of rays whose wavelengths and
energy are determined by the nature of
the source.
2. Each of the commonly used
radioisotopes has a specific application
because of the fixed gamma energy
characteristics.
1. Radiation from a gamma ray source
consists of rays whose wavelengths and
energy are determined by the nature of
the source.
2. Each of the commonly used
radioisotopes has a specific application
because of the fixed gamma energy
characteristics.
Gamma Ray Quality CharacteristicsGamma Ray Quality Characteristics
3. The table on the next slide lists the most common radioisotopes for radiography and their equivalent energy.
3. The table on the next slide lists the most common radioisotopes for radiography and their equivalent energy.
Gamma Ray Quality CharacteristicsGamma Ray Quality Characteristics
4. Gamma rays and X-rays have identical propagation characteristics, and both conform to the inverse square law.
5. The mechanism of interaction of gamma rays with matter is identical to those discussed for X-rays.
4. Gamma rays and X-rays have identical propagation characteristics, and both conform to the inverse square law.
5. The mechanism of interaction of gamma rays with matter is identical to those discussed for X-rays.
Lesson 3Lesson 3
EquipmentEquipment
X-Ray EquipmentX-Ray Equipment
There are three basic requirements
for the generation of X-rays:
1. A source of free electrons.
1. A means of rapidly accelerating
the beam of electrons.
2. A suitable target material to stop
the electrons.
There are three basic requirements
for the generation of X-rays:
1. A source of free electrons.
1. A means of rapidly accelerating
the beam of electrons.
2. A suitable target material to stop
the electrons.
Portable X-Ray UnitsPortable X-Ray Units
In field radiography (inspection of
pipelines, bridges, vessels, and
ships), portable X-ray units are very
important. The characteristic of these
tubes are:
1. Light weight.
2. Compact.
3. Usually air cooled.
In field radiography (inspection of
pipelines, bridges, vessels, and
ships), portable X-ray units are very
important. The characteristic of these
tubes are:
1. Light weight.
2. Compact.
3. Usually air cooled.
X-Ray TubeX-Ray Tube
The main components of any X-ray equipment are:
1. Tube: Enclosed in a high vacuum envelope of heat resistant glass or ceramic.
2. Cathode: To produce free electros.
3. Anode: Target which the electrodes strike.
The main components of any X-ray equipment are:
1. Tube: Enclosed in a high vacuum envelope of heat resistant glass or ceramic.
2. Cathode: To produce free electros.
3. Anode: Target which the electrodes strike.
X-Ray TubeX-Ray Tube
Associated with the tube are the following parts:
1. Equipment that heats the filament, accelerates, and controls the resultant free electrons.
2. Equipment to remove the heat generated by the X-rays.
3. Shielding of the equipment.
Associated with the tube are the following parts:
1. Equipment that heats the filament, accelerates, and controls the resultant free electrons.
2. Equipment to remove the heat generated by the X-rays.
3. Shielding of the equipment.
X-Ray TubeX-Ray Tube
There are many varieties in the
size and shape of X-ray tubes.
There are many varieties in the
size and shape of X-ray tubes.
Tube EnvelopeTube Envelope
1. Tube envelope is constructed of
glass or ceramic that has:
a. A high melting point.
b. Sufficient strength.
2. For the following reasons, a high
vacuum environment for the tube
element is necessary.
1. Tube envelope is constructed of
glass or ceramic that has:
a. A high melting point.
b. Sufficient strength.
2. For the following reasons, a high
vacuum environment for the tube
element is necessary.
Tube EnvelopeTube Envelope
a. Preventing oxidation of the
electrode material.
b. Permits ready passage of the
electron beam without ionization of
gas within the tube.
c. Provides electrical insulation
between the electrodes.
a. Preventing oxidation of the
electrode material.
b. Permits ready passage of the
electron beam without ionization of
gas within the tube.
c. Provides electrical insulation
between the electrodes.
CathodeCathode
Cathode of X-ray tubes consists of:
1. Focusing cup: Functions
as an electrostatic lens.
2. Filament: A coil of tungsten
wire that produces a cloud
of electrons by flowing an
electrical current through it.
Cathode of X-ray tubes consists of:
1. Focusing cup: Functions
as an electrostatic lens.
2. Filament: A coil of tungsten
wire that produces a cloud
of electrons by flowing an
electrical current through it.
Filament HeatingFilament Heating
1. A small flow of current through the filament is enough to heat it to a temperature that causes electron emission.
2. A change in the number of emitted electrons varies with the current flow through the filament.
3. The tube current is measured in milliamperes (mA), and it controls the intensity of X-rays.
1. A small flow of current through the filament is enough to heat it to a temperature that causes electron emission.
2. A change in the number of emitted electrons varies with the current flow through the filament.
3. The tube current is measured in milliamperes (mA), and it controls the intensity of X-rays.
Anode and CathodeAnode and Cathode
1. The anode of X-ray tube is
usually made of copper.
2. Copper and tungsten are the
most common anode materials.
1. The anode of X-ray tube is
usually made of copper.
2. Copper and tungsten are the
most common anode materials.
AnodeAnode
3. A dense target material is
required to ensure a maximum
number of collisions.
4. Material with a high melting point
is necessary for a target to
withstand the excessive heat.
3. A dense target material is
required to ensure a maximum
number of collisions.
4. Material with a high melting point
is necessary for a target to
withstand the excessive heat.
Focal SpotFocal Spot
1. The image sharpness is partly determined by the size of the focal spot.
2. The electron beam is focused so that a rectangular area of the target is bombarded by the beam.
1. The image sharpness is partly determined by the size of the focal spot.
2. The electron beam is focused so that a rectangular area of the target is bombarded by the beam.
Focal SpotFocal Spot
3. The projected area of the electron beam is the effective focal spot (as seen in the following slide).
4. The size to which the focal spot can be reduced is limited by the heat generated in target bombardment.
3. The projected area of the electron beam is the effective focal spot (as seen in the following slide).
4. The size to which the focal spot can be reduced is limited by the heat generated in target bombardment.
Linear AcceleratorsLinear Accelerators
There are two types of linear
accelerators:
1. Standing wave linear accelerator for energy up to 200 MeV.
2. Traveling wave linear accelerator for energy up to 30 GeV (giga-electron volts, or billion electron volts).
There are two types of linear
accelerators:
1. Standing wave linear accelerator for energy up to 200 MeV.
2. Traveling wave linear accelerator for energy up to 30 GeV (giga-electron volts, or billion electron volts).
X-Ray Beam ConfigurationX-Ray Beam Configuration
1. Once the X-rays are created, they
cannot be focused or otherwise
directed.
2. The direction of useful X-radiation
is determined by the positioning of
the target and the lead shielding.
1. Once the X-rays are created, they
cannot be focused or otherwise
directed.
2. The direction of useful X-radiation
is determined by the positioning of
the target and the lead shielding.
Accelerating PotentialAccelerating Potential
1. The applied potential between the
cathode and anode determines the
penetrating effect of the produced X-
ray.
2. The higher the voltage, the greater the
electron velocity and the shorter
wavelengths and more penetrating
power for the generated X-rays.
1. The applied potential between the
cathode and anode determines the
penetrating effect of the produced X-
ray.
2. The higher the voltage, the greater the
electron velocity and the shorter
wavelengths and more penetrating
power for the generated X-rays.
Iron Core TransformersIron Core Transformers
1. The majority of X-ray equipment
for industrial radiography (up to
400 kV) use iron core
transformers.
2. Their basic limitations are their
size and weight.
1. The majority of X-ray equipment
for industrial radiography (up to
400 kV) use iron core
transformers.
2. Their basic limitations are their
size and weight.
Heat DissipationHeat Dissipation
1. X-ray generation is a very
inefficient process; most of the
electron energy is expended in
producing heat.
2. Heat dissipation in the X-ray tube is
done by a flow of oil, gas or water.
1. X-ray generation is a very
inefficient process; most of the
electron energy is expended in
producing heat.
2. Heat dissipation in the X-ray tube is
done by a flow of oil, gas or water.
Heat DissipationHeat Dissipation
3. Efficiency of an X-ray tube
cooling system is the main factor
in determining the duty cycle of
the tube.
3. Efficiency of an X-ray tube
cooling system is the main factor
in determining the duty cycle of
the tube.
Equipment ShieldingEquipment Shielding
1. To prevent unwanted radiation, lead is used to shield the X-ray tube.
2. The design of this shielding varies with different X-ray tubes, but in all cases, it serves to absorb that portion of the radiation that is not traveling in the desired direction.
1. To prevent unwanted radiation, lead is used to shield the X-ray tube.
2. The design of this shielding varies with different X-ray tubes, but in all cases, it serves to absorb that portion of the radiation that is not traveling in the desired direction.
Control PanelControl Panel
1. The control panel of an X-ray system is designed to permit a radiographer to set the desired exposure parameters.
2. The control panel also provides critical indications for tube performance, such as cooling system, flow of cooling oil, or water.
1. The control panel of an X-ray system is designed to permit a radiographer to set the desired exposure parameters.
2. The control panel also provides critical indications for tube performance, such as cooling system, flow of cooling oil, or water.
Gamma Ray EquipmentGamma Ray Equipment
1. Handling and storage of gamma ray sources are extremely important due to the fact they cannot be shut off.
2. The United State Nuclear Regulatory Commission (NRC) and various state agencies recommend safety standards for proper transportation, storage and handling of radioisotopes.
1. Handling and storage of gamma ray sources are extremely important due to the fact they cannot be shut off.
2. The United State Nuclear Regulatory Commission (NRC) and various state agencies recommend safety standards for proper transportation, storage and handling of radioisotopes.
Gamma Ray SourcesGamma Ray Sources
1. There are two types of gamma ray sources:
a. Natural isotopes.
b. Artificial isotopes.
2. Most isotopes used in industrial radiography are round wafers encapsulated in a stainless steel cylinder.
1. There are two types of gamma ray sources:
a. Natural isotopes.
b. Artificial isotopes.
2. Most isotopes used in industrial radiography are round wafers encapsulated in a stainless steel cylinder.
RadiumRadium
1. Radium is a natural radioactive
substance having a half life of
about 1600 years.
2. Most radium sources consist of
radium sulfate packaged in
either spherical or cylindrical
capsules.
1. Radium is a natural radioactive
substance having a half life of
about 1600 years.
2. Most radium sources consist of
radium sulfate packaged in
either spherical or cylindrical
capsules.
RadiumRadium
3. Because of its low specific
activity and its long half life,
radium is rarely used in industrial
radiography.
3. Because of its low specific
activity and its long half life,
radium is rarely used in industrial
radiography.
Artificial RadioisotopesArtificial Radioisotopes
1. The artificial radioisotopes used in industrial radiography or gauging purposes are:
1. Cobalt-60 (Co-60).
2. Iridium-192 (Ir-192).
3. Selenium-75 (Se-75).
4. Thulium-170 (Tm-170).
5. Cesium-137 (Cs-137).
1. The artificial radioisotopes used in industrial radiography or gauging purposes are:
1. Cobalt-60 (Co-60).
2. Iridium-192 (Ir-192).
3. Selenium-75 (Se-75).
4. Thulium-170 (Tm-170).
5. Cesium-137 (Cs-137).
Artificial RadioisotopesArtificial Radioisotopes
2. The following table gives a
summary of the main
characteristics of the most used
isotopes.
2. The following table gives a
summary of the main
characteristics of the most used
isotopes.
Radioisotope characteristicsRadioisotope characteristics
Isotope CamerasIsotope Cameras
1. The equipment to accomplish safe handling and storage of radioisotopes is called a camera or exposure device.
2. These cameras are self contained units, meaning no external power supply is required.
1. The equipment to accomplish safe handling and storage of radioisotopes is called a camera or exposure device.
2. These cameras are self contained units, meaning no external power supply is required.
Isotope CamerasIsotope Cameras
3. The exposure devices contain
self locking mechanisms
ensuring safety in accordance
with ANSI and ISO requirements,
in addition to NRC and IAEA
requirements.
3. The exposure devices contain
self locking mechanisms
ensuring safety in accordance
with ANSI and ISO requirements,
in addition to NRC and IAEA
requirements.
Lesson 4Lesson 4
Radiographic FilmRadiographic Film
IntroductionIntroduction
1. Radiographic film consists of:
a. Base: A thin, transparent plastic sheet.
b. Emulsion coat: Coat of an emulsion of gelatin on one or both sides about 0.001 in. (0.003 cm) thick. The emulsion coat contains very fine grains of silver bromide (AgBr).
1. Radiographic film consists of:
a. Base: A thin, transparent plastic sheet.
b. Emulsion coat: Coat of an emulsion of gelatin on one or both sides about 0.001 in. (0.003 cm) thick. The emulsion coat contains very fine grains of silver bromide (AgBr).
IntroductionIntroduction
2. Latent (hidden) image:
Exposure of radiation on the film
that cannot be detected until
chemical processing occurs.
3. Visible image: Image on the
film after developed by chemical
processing.
2. Latent (hidden) image:
Exposure of radiation on the film
that cannot be detected until
chemical processing occurs.
3. Visible image: Image on the
film after developed by chemical
processing.
Usefulness of RadiographsUsefulness of Radiographs
1. Film density: Degree of darkening
on the developed film.
2. Radiographic contrast:
Difference between two film areas.
Darker area (higher density) has
received more radiation compared
to the area of light density.
1. Film density: Degree of darkening
on the developed film.
2. Radiographic contrast:
Difference between two film areas.
Darker area (higher density) has
received more radiation compared
to the area of light density.
Usefulness of RadiographsUsefulness of Radiographs
3. Definition: Sharpness of any
change in film density.
4. Contrast and definition are
important for a successful
interpretation of radiographs.
3. Definition: Sharpness of any
change in film density.
4. Contrast and definition are
important for a successful
interpretation of radiographs.
Radiographic ContrastRadiographic Contrast
1. The film density D is logarithmic value
defined as:
D = log10 (I0/I)
where (I0) is the intensity of the incident
light to view the film, and I is the intensity
of the transmitted light through the film.
The higher the number, the darker the
film.
1. The film density D is logarithmic value
defined as:
D = log10 (I0/I)
where (I0) is the intensity of the incident
light to view the film, and I is the intensity
of the transmitted light through the film.
The higher the number, the darker the
film.
Radiographic ContrastRadiographic Contrast
2. If the intensity of light is 1000
units and the film allows only
one unit of that intensity to pass
through, the film density based
on the previous equation will be:
D = log10 (1000/1) = 3
2. If the intensity of light is 1000
units and the film allows only
one unit of that intensity to pass
through, the film density based
on the previous equation will be:
D = log10 (1000/1) = 3
Radiographic ContrastRadiographic Contrast
3. Radiographic contrast (as shown
in the following figure) is defined
as the difference in the film
density between two selected
areas of the exposed and
developed film.
3. Radiographic contrast (as shown
in the following figure) is defined
as the difference in the film
density between two selected
areas of the exposed and
developed film.
Radiographic ContrastRadiographic Contrast
4. Higher contrast is better for film
interpretation.
5. Radiographic contrast is a
combination of:
a. Subject contrast.
b. Film contrast.
4. Higher contrast is better for film
interpretation.
5. Radiographic contrast is a
combination of:
a. Subject contrast.
b. Film contrast.
Radiographic ContrastRadiographic Contrast
6. Radiographic contrast depends on:
a. Applied radiation energy (penetrating quality).
b. Contrast characteristics of the film.
c. Amount of exposure (the product of radiation intensity and exposure time).
6. Radiographic contrast depends on:
a. Applied radiation energy (penetrating quality).
b. Contrast characteristics of the film.
c. Amount of exposure (the product of radiation intensity and exposure time).
Radiographic ContrastRadiographic Contrast
d. Film screen.
e. Film processing.
f. Scattered radiation.
d. Film screen.
e. Film processing.
f. Scattered radiation.
Subject ContrastSubject Contrast
1. Subject contrast is the relative
radiation intensities passing
through any two selected
portions of material. Subject
contrast depends on the
following factors:
1. Subject contrast is the relative
radiation intensities passing
through any two selected
portions of material. Subject
contrast depends on the
following factors:
Subject ContrastSubject Contrast
a. Type and shape of the test object.
b. Energy of the applied energy
radiation wavelength, type of
source.
c. Scattered radiation.
a. Type and shape of the test object.
b. Energy of the applied energy
radiation wavelength, type of
source.
c. Scattered radiation.
Subject ContrastSubject Contrast
2. Subject contrast decreases as
the wavelength of the incident
radiation decreases.
2. Subject contrast decreases as
the wavelength of the incident
radiation decreases.
Subject ContrastSubject Contrast
3. Higher subject contrast can be achieved by:
a. Larger thickness variation.
b. Use of different X-ray or gamma ray energies.
c. Masks.
d. Diaphragms.
e. Filters or screens.
3. Higher subject contrast can be achieved by:
a. Larger thickness variation.
b. Use of different X-ray or gamma ray energies.
c. Masks.
d. Diaphragms.
e. Filters or screens.
Film ContrastFilm Contrast
1. The ability of film to detect and
record different radiation
exposures as differences in film
density is called film contrast.
1. The ability of film to detect and
record different radiation
exposures as differences in film
density is called film contrast.
Film ContrastFilm Contrast
2. The relationship between the
amount of exposure and the
resulting film density is
expressed in the form of film
characteristic curves and is
determined by the following
factors:
2. The relationship between the
amount of exposure and the
resulting film density is
expressed in the form of film
characteristic curves and is
determined by the following
factors:
Film ContrastFilm Contrast
a. Film grain size.
b. Chemistry of the film processing chemical.
c. Concentration of the processing chemicals.
d. Development time.
e. Development temperature.
f. Agitation in the developer solution.
a. Film grain size.
b. Chemistry of the film processing chemical.
c. Concentration of the processing chemicals.
d. Development time.
e. Development temperature.
f. Agitation in the developer solution.
Film Characteristic CurvesFilm Characteristic Curves
1. The following figure shows a film characteristic curve.
a. The vertical axis is the resulting film density.
b. The horizontal axis is expressed in a logarithm of relative exposure.
1. The following figure shows a film characteristic curve.
a. The vertical axis is the resulting film density.
b. The horizontal axis is expressed in a logarithm of relative exposure.
Film Characteristic CurvesFilm Characteristic Curves
c. The minimum point of the curve
on the vertical axis is called fog
density.
d. Based on this curve, as the
exposure increases, film contrast
increases.
c. The minimum point of the curve
on the vertical axis is called fog
density.
d. Based on this curve, as the
exposure increases, film contrast
increases.
Film Characteristic CurvesFilm Characteristic Curves
2. A film characteristic curve has
two different sections:
a. A tail of lower densities.
b. A straighter portion (with
a higher slope on the
curve).
2. A film characteristic curve has
two different sections:
a. A tail of lower densities.
b. A straighter portion (with
a higher slope on the
curve).
Film Characteristic CurvesFilm Characteristic Curves
3. High radiographic contrast is
achieved with densities at the
straight portion of a characteristic
curve. This is the reason that
films should always be exposed
for a density of at least 1.5.
3. High radiographic contrast is
achieved with densities at the
straight portion of a characteristic
curve. This is the reason that
films should always be exposed
for a density of at least 1.5.
Film Characteristic CurvesFilm Characteristic Curves
4. Most radiographic codes,
standards and specifications
usually give upper and lower
density limits within a range of
1.8 to 4.0.
4. Most radiographic codes,
standards and specifications
usually give upper and lower
density limits within a range of
1.8 to 4.0.
Film SpeedFilm Speed
1. Film speed is an important
consideration in determining the
proper exposure time to obtain the
desired film density.
2. The next figure illustrates films with
high, medium and low speeds.
1. Film speed is an important
consideration in determining the
proper exposure time to obtain the
desired film density.
2. The next figure illustrates films with
high, medium and low speeds.
Film SpeedFilm Speed
3. Knowing film speed is important
in film selection for each
particular radiographic testing
task.
3. Knowing film speed is important
in film selection for each
particular radiographic testing
task.
GraininessGraininess
1. Graininess is the visible evidence of
the grouping into clumps of the silver
particles that form the image on the
radiographic film.
2. The following figure shows the effect
of grain variation on the image
definition.
1. Graininess is the visible evidence of
the grouping into clumps of the silver
particles that form the image on the
radiographic film.
2. The following figure shows the effect
of grain variation on the image
definition.
GraininessGraininess
3. The degree of graininess of an
exposed film depends on the
following factors:
a. Grain size.
b. The quality of the radiation.
c. Film process conditions.
d. Type of film screens.
3. The degree of graininess of an
exposed film depends on the
following factors:
a. Grain size.
b. The quality of the radiation.
c. Film process conditions.
d. Type of film screens.
Film Selection FactorsFilm Selection Factors
1. When not otherwise specified by the
customer or governing standards, the
selection of film is made by the
radiographer. Most of the time, the
selection of film is based on the
following factors:
a. Need for certain contrast and
definition quality.
1. When not otherwise specified by the
customer or governing standards, the
selection of film is made by the
radiographer. Most of the time, the
selection of film is based on the
following factors:
a. Need for certain contrast and
definition quality.
Film Selection FactorsFilm Selection Factors
b. Thickness and density of the test
object.
c. The type of indication or
discontinuity normally associated
with the object.
d. Size of an acceptable indication.
b. Thickness and density of the test
object.
c. The type of indication or
discontinuity normally associated
with the object.
d. Size of an acceptable indication.
Film Selection FactorsFilm Selection Factors
e. Accessibility, location and
configuration of the test object.
f. Customer requirements.
e. Accessibility, location and
configuration of the test object.
f. Customer requirements.
Film Selection FactorsFilm Selection Factors
2. In film selection, remember that:
a. Film contrast, film speed and
graininess are interrelated.
b. Faster films need shorter
exposure time, but usually
have larger grains and poor
resolution/sensitivity.
2. In film selection, remember that:
a. Film contrast, film speed and
graininess are interrelated.
b. Faster films need shorter
exposure time, but usually
have larger grains and poor
resolution/sensitivity.
Film Selection FactorsFilm Selection Factors
c. Slower films need longer
exposure time, but have finer
grain and good resolution/
sensitivity.
c. Slower films need longer
exposure time, but have finer
grain and good resolution/
sensitivity.
Film Selection FactorsFilm Selection Factors
d. Film manufacturers’
recommendations for film
selection are a useful tool in
selecting the proper film for a
given application.
d. Film manufacturers’
recommendations for film
selection are a useful tool in
selecting the proper film for a
given application.
Film ProcessingFilm Processing
1. Film processing makes the latent
image visible.
2. The following general
precautions must be observed
during film processing:
1. Film processing makes the latent
image visible.
2. The following general
precautions must be observed
during film processing:
Film ProcessingFilm Processing
a. Follow manufacturer recommendations
for chemical concentrations, temperature
and processing time.
b. Use equipment, tanks, trays and holders
that can withstand the chemical action.
a. Follow manufacturer recommendations
for chemical concentrations, temperature
and processing time.
b. Use equipment, tanks, trays and holders
that can withstand the chemical action.
Film ProcessingFilm Processing
c. Ensure tanks are clean.
d. Recommended safelights should
be used and should be checked
regularly.
c. Ensure tanks are clean.
d. Recommended safelights should
be used and should be checked
regularly.
Film ProcessingFilm Processing
e. Maintain cleanliness in the
darkroom to avoid any artifacts
on developed radiographs.
f. Avoid any contamination of
different solutions.
e. Maintain cleanliness in the
darkroom to avoid any artifacts
on developed radiographs.
f. Avoid any contamination of
different solutions.
Tank ProcessingTank Processing
The arrangement of tank processing
(manual processing) unit is shown in
the next slide.
The arrangement of tank processing
(manual processing) unit is shown in
the next slide.
Tank ProcessingTank Processing
1. The tanks for processing solutions and
wash water should be deep enough for
the film to be submerged.
2. The chemicals in the tanks must be
stirred and the temperature must be
checked with calibrated thermometer
before turning off the ambient light.
1. The tanks for processing solutions and
wash water should be deep enough for
the film to be submerged.
2. The chemicals in the tanks must be
stirred and the temperature must be
checked with calibrated thermometer
before turning off the ambient light.
Tank ProcessingTank Processing
3. All required equipment should be
arranged before turning off the
ambient light.
4. All unnecessary materials should
be kept away from the
processing area.
3. All required equipment should be
arranged before turning off the
ambient light.
4. All unnecessary materials should
be kept away from the
processing area.
Tank ProcessingTank Processing
5. Test the safe lights and arrangement
them for easy viewing. Follow the
standard recommendations for
regular checking.
6. The door to the darkroom should be
locked to prevent accidental
exposure to ambient light.
5. Test the safe lights and arrangement
them for easy viewing. Follow the
standard recommendations for
regular checking.
6. The door to the darkroom should be
locked to prevent accidental
exposure to ambient light.
Tank ProcessingTank Processing
7. To load the film inside the hangers, it
should grasped by its edges or corner
to avoid finger prints, bending,
wrinkling or crimping during handling.
8. Keep the loading area completely dry.
9. Follow the tank processing
procedures.
7. To load the film inside the hangers, it
should grasped by its edges or corner
to avoid finger prints, bending,
wrinkling or crimping during handling.
8. Keep the loading area completely dry.
9. Follow the tank processing
procedures.
Tank Processing FeaturesTank Processing Features
There are five separate steps in tank processing:
1. Developing.
2. Stop bath.
3. Fixing.
4. Washing.
5. Drying.
There are five separate steps in tank processing:
1. Developing.
2. Stop bath.
3. Fixing.
4. Washing.
5. Drying.
DevelopingDeveloping
Developing is the chemical
process of reducing silver
bromide particles in the exposed
area of the film emulsion to
metallic silver.
Developing is the chemical
process of reducing silver
bromide particles in the exposed
area of the film emulsion to
metallic silver.
DevelopingDeveloping
1. Follow the manufacturers’
recommendations for developing
temperature and time.
2. Film should be agitated during
developing to obtain a uniform
development and to avoid any air
bubbles from attaching to the film.
1. Follow the manufacturers’
recommendations for developing
temperature and time.
2. Film should be agitated during
developing to obtain a uniform
development and to avoid any air
bubbles from attaching to the film.
DevelopingDeveloping
3. Use strips of exposed radiographs
to control the developer activity as
regular quality control checking.
4. Follow the manufacturers’
recommendations to replenish the
solution.
3. Use strips of exposed radiographs
to control the developer activity as
regular quality control checking.
4. Follow the manufacturers’
recommendations to replenish the
solution.
Stop BathStop Bath
The stop bath, a solution of acetic acid
and water, serves to remove the residual
developer solution from the film.
1. Uncontaminated running water for at
least 2 min can be used as an
alternative to stop bath.
The stop bath, a solution of acetic acid
and water, serves to remove the residual
developer solution from the film.
1. Uncontaminated running water for at
least 2 min can be used as an
alternative to stop bath.
Stop BathStop Bath
2. Manufacturers’ directions should
be used to make the stop bath
solution.
3. A fresh stop bath solution is
yellow in color and clear under
safelight.
2. Manufacturers’ directions should
be used to make the stop bath
solution.
3. A fresh stop bath solution is
yellow in color and clear under
safelight.
FixingFixing
1. Fixer, an acidic solution, has two
functions on the film:
a. It dissolves and removes the
silver bromide from the
undeveloped portions of the film
without affecting the
developed portion.
b. It hardens the emulsion gelatin.
1. Fixer, an acidic solution, has two
functions on the film:
a. It dissolves and removes the
silver bromide from the
undeveloped portions of the film
without affecting the
developed portion.
b. It hardens the emulsion gelatin.
FixingFixing
2. The minimum time required for
fixing is twice the amount of time
necessary to clean the film.
3. Fixing time should not exceed 15
min.
4. Improper fixing shortens the
archival length of the film.
2. The minimum time required for
fixing is twice the amount of time
necessary to clean the film.
3. Fixing time should not exceed 15
min.
4. Improper fixing shortens the
archival length of the film.
FixingFixing
5. Film should be agitated in fixing
solution at 2 min intervals.
6. The replacement of fixing
solution should be determined by
checking the acidity of the
solution.
5. Film should be agitated in fixing
solution at 2 min intervals.
6. The replacement of fixing
solution should be determined by
checking the acidity of the
solution.
WashingWashing
After fixing, washing is necessary to
remove the fixer from the emulsion.
1. Each film is washed for a period
of time equal to twice the fixing.
2. Hypo clearing agent may be
used to speed up film washing.
After fixing, washing is necessary to
remove the fixer from the emulsion.
1. Each film is washed for a period
of time equal to twice the fixing.
2. Hypo clearing agent may be
used to speed up film washing.
WashingWashing
3. Best results for washing are
obtained with a water temperature
between 65 and 70° F (18.3 and
21.1° C).
4. To avoid any water marks, film is
immersed in a wetting agent that
also aids in reducing the drying
time.
3. Best results for washing are
obtained with a water temperature
between 65 and 70° F (18.3 and
21.1° C).
4. To avoid any water marks, film is
immersed in a wetting agent that
also aids in reducing the drying
time.
DryingDrying
The final stage of the film
processing is drying.
The final stage of the film
processing is drying.
Automatic Film ProcessingAutomatic Film Processing
Automatic film processing
systems are used whenever the
volume of work makes them
economical.
Automatic film processing
systems are used whenever the
volume of work makes them
economical.
Automatic Film ProcessingAutomatic Film Processing
1. The entire processing cycles is
completed in less than 15 min.
2. Automatic film processing units
consistently produce radiographs
of much higher quality than a
manual one.
1. The entire processing cycles is
completed in less than 15 min.
2. Automatic film processing units
consistently produce radiographs
of much higher quality than a
manual one.
Automatic Film ProcessingAutomatic Film Processing
3. Loading the film inside the unit
should be done in a dark
environment.
4. Properly maintaining the system
is the key for high performance
of an automatic system.
3. Loading the film inside the unit
should be done in a dark
environment.
4. Properly maintaining the system
is the key for high performance
of an automatic system.
Darkroom Facilities and EquipmentDarkroom Facilities and Equipment
Some requirements that must be satisfied in the design and construction of a darkroom:
1. It must be lighted with suitable and tested safelights.
2. It must be protected against ambient light from outside sources.
3. The walls and ceiling must be painted with lightly-colored, semi- gloss paint.
Some requirements that must be satisfied in the design and construction of a darkroom:
1. It must be lighted with suitable and tested safelights.
2. It must be protected against ambient light from outside sources.
3. The walls and ceiling must be painted with lightly-colored, semi- gloss paint.
Darkroom Facilities and EquipmentDarkroom Facilities and Equipment
4. Darkroom floors are usually covered with chemical resistant, water-proof and slip-proof materials.
5. Cleanliness is of great importance during the entire film processing procedure.
4. Darkroom floors are usually covered with chemical resistant, water-proof and slip-proof materials.
5. Cleanliness is of great importance during the entire film processing procedure.
Radiographic FilmRadiographic Film
1. Radiographic film consists of:
a. Base: A thin, transparent plastic sheet.
b. Emulsion coat: Coat of an emulsion of gelatin on one or both sides about 0.001 in.
(0.003 cm) thick. The emulsion coat contains very fine grains of silver bromide (AgBr).
1. Radiographic film consists of:
a. Base: A thin, transparent plastic sheet.
b. Emulsion coat: Coat of an emulsion of gelatin on one or both sides about 0.001 in.
(0.003 cm) thick. The emulsion coat contains very fine grains of silver bromide (AgBr).
Radiographic FilmRadiographic Film
2. Latent (hidden) image: Trace of
exposure of radiation on the exposed
film, cannot be detected by ordinary
physical methods.
3. Visible image: Image on the film after
developed by chemical processing.
2. Latent (hidden) image: Trace of
exposure of radiation on the exposed
film, cannot be detected by ordinary
physical methods.
3. Visible image: Image on the film after
developed by chemical processing.
Lesson 5Lesson 5
SafetySafety
IntroductionIntroduction
1. Radiographers are cautioned to
be aware of the latest effective
safety regulations.
2. Radiation safety practices are
based on the effects of radiation
on the human body, and
characteristics of radiation.
1. Radiographers are cautioned to
be aware of the latest effective
safety regulations.
2. Radiation safety practices are
based on the effects of radiation
on the human body, and
characteristics of radiation.
IntroductionIntroduction
3. Personnel protection is
dependant upon detection
devices, and through the proper
use of time, distance and
shielding.
3. Personnel protection is
dependant upon detection
devices, and through the proper
use of time, distance and
shielding.
IntroductionIntroduction
4. Agreement States are the
regulations covering use, handling
and transportation of radioactive
materials approved by the Nuclear
Regulatory Commission (NRC).
4. Agreement States are the
regulations covering use, handling
and transportation of radioactive
materials approved by the Nuclear
Regulatory Commission (NRC).
IntroductionIntroduction
5. All of the safety regulations are
designed to limit exposure to the
radiographer and to provide
protection to the general public.
5. All of the safety regulations are
designed to limit exposure to the
radiographer and to provide
protection to the general public.
IntroductionIntroduction
6. The radiographer, who is
employed by a licensee of NRC
or who is employed by a
licensee of an agreement state,
must have knowledge of, and
comply with, all applicable
regulations.
6. The radiographer, who is
employed by a licensee of NRC
or who is employed by a
licensee of an agreement state,
must have knowledge of, and
comply with, all applicable
regulations.
Units of Radiation Dose MeasurementUnits of Radiation Dose Measurement
1. The damaging effects of
radiation are dependent on both
the type and the level of energy
of the radiation.
2. For different types of radiation, a
relative biological effectiveness
is applied.
1. The damaging effects of
radiation are dependent on both
the type and the level of energy
of the radiation.
2. For different types of radiation, a
relative biological effectiveness
is applied.
Units of Radiation Dose MeasurementUnits of Radiation Dose Measurement
3. For radiation safety purposes,
the cumulative effect of radiation
on the human body is of primary
concerns.
3. For radiation safety purposes,
the cumulative effect of radiation
on the human body is of primary
concerns.
Roentgen (R)Roentgen (R)
1. The roentgen (R) or sievert (Sv) is
the physical unit measure of the
ionization of air by X-radiation or
gamma radiation.
1. The roentgen (R) or sievert (Sv) is
the physical unit measure of the
ionization of air by X-radiation or
gamma radiation.
Roentgen (R)Roentgen (R)
2. It is defined as the quantity of
radiation that will produce one
electrostatic unit (esu) of charge
in one cubic centimeter of air at
standard pressure and
temperature (STP).
2. It is defined as the quantity of
radiation that will produce one
electrostatic unit (esu) of charge
in one cubic centimeter of air at
standard pressure and
temperature (STP).
Roentgen (R)Roentgen (R)
3. 1 R of radiation = absorption by
ionization of about 83 erg (unit of
work or energy in physics) of
radiation energy per gram of air.
4. For practical purpose, mR is often
used, which is:
1 mR = 1/1000 R.
3. 1 R of radiation = absorption by
ionization of about 83 erg (unit of
work or energy in physics) of
radiation energy per gram of air.
4. For practical purpose, mR is often
used, which is:
1 mR = 1/1000 R.
Radiation Absorbed Dose (rad)Radiation Absorbed Dose (rad)
1. Radiation absorbed dose (rad) is
the unit of measurement of
radiation absorption by humans.
2. It represents an absorption of
100 erg of energy per gram of
irradiated tissue.
1. Radiation absorbed dose (rad) is
the unit of measurement of
radiation absorption by humans.
2. It represents an absorption of
100 erg of energy per gram of
irradiated tissue.
Radiation Absorbed Dose (rad)Radiation Absorbed Dose (rad)
3. Whereas the roentgen applies only
to X-rays and gamma rays, radiation
absorbed dose applies to any type of
radiations
4. For X-ray and gamma radiation,
exposure to 1 R results in 1 rad.
3. Whereas the roentgen applies only
to X-rays and gamma rays, radiation
absorbed dose applies to any type of
radiations
4. For X-ray and gamma radiation,
exposure to 1 R results in 1 rad.
Radiation Absorbed Dose (rad)Radiation Absorbed Dose (rad)
5. The unit gray (Gy) has been
introduced as: 100 rad = 1 Gy.
5. The unit gray (Gy) has been
introduced as: 100 rad = 1 Gy.
Quality FactorQuality Factor
1. Quality factor takes into account the
biological effect of different
radiations on human body.
1. Quality factor takes into account the
biological effect of different
radiations on human body.
Quality FactorQuality Factor
2. Quality factor values are
determined by National
Committee on Radiation
Protection. They are summarized
in the following table.
2. Quality factor values are
determined by National
Committee on Radiation
Protection. They are summarized
in the following table.
Roentgen Equivalent Man (rem)Roentgen Equivalent Man (rem)
1. Roentgen equivalent man (rem)
represents the absorbed dose in
radiation absorbed dose (rad),
multiplied by the quality factor of the
type of radiation.
2. Radiation safety levels are
established in terms of roentgen
equivalent man (rem).
1. Roentgen equivalent man (rem)
represents the absorbed dose in
radiation absorbed dose (rad),
multiplied by the quality factor of the
type of radiation.
2. Radiation safety levels are
established in terms of roentgen
equivalent man (rem).
Roentgen Equivalent Man (rem)Roentgen Equivalent Man (rem)
3. Since the quality factor of
X-radiation and gamma radiation
is one, then:
1 rad = 1 rem.
3. Since the quality factor of
X-radiation and gamma radiation
is one, then:
1 rad = 1 rem.
International System of Units (SI) Measurements
International System of Units (SI) Measurements
1. The Nuclear Regulatory
Commission, state regulations
and radiographers in the US
often still use the old English
units: curie, roentgen, rem and
rad.
1. The Nuclear Regulatory
Commission, state regulations
and radiographers in the US
often still use the old English
units: curie, roentgen, rem and
rad.
International System of Units (SI) Measurements
International System of Units (SI) Measurements
2. Different organizations like The National
Institute of Standards & Technology
(NIST), The American National
Standards Institute (ANSI), The
American Society for Testing and
Materials (ASTM), The Institute of
Electrical and Electronics Engineers
(IEEE), …
2. Different organizations like The National
Institute of Standards & Technology
(NIST), The American National
Standards Institute (ANSI), The
American Society for Testing and
Materials (ASTM), The Institute of
Electrical and Electronics Engineers
(IEEE), …
International System of Units (SI) Measurements
International System of Units (SI) Measurements
… the International Organization for
Standardization (ISO) and The
American Society for
Nondestructive Testing (ASNT)
all support the replacement of
older units with SI units.
… the International Organization for
Standardization (ISO) and The
American Society for
Nondestructive Testing (ASNT)
all support the replacement of
older units with SI units.
Becquerel Replaces CurieBecquerel Replaces Curie
1. Curie (Ci) is the original unit for
radioactivity, which is defined as:
3.7 X 1010 disintegrations per
second.
2. In SI, the replace unit for
radioactivity is the becquerel (Bq),
which is one disintegration per
second.
1. Curie (Ci) is the original unit for
radioactivity, which is defined as:
3.7 X 1010 disintegrations per
second.
2. In SI, the replace unit for
radioactivity is the becquerel (Bq),
which is one disintegration per
second.
Becquerel Replaces CurieBecquerel Replaces Curie
3. 1 Ci = 37 GBq (gigabecquerel),
where giga = 109.
3. 1 Ci = 37 GBq (gigabecquerel),
where giga = 109.
Coulomb per Kilogram Replaces Roentgen
Coulomb per Kilogram Replaces Roentgen
1. Coulomb (C) is the unit of
electrical change, where:
1 C = 1 ampere X 1 second.
2. 1 R = 258 microcoulombs per
kilogram of air (258 µC·kg–1 of
air).
1. Coulomb (C) is the unit of
electrical change, where:
1 C = 1 ampere X 1 second.
2. 1 R = 258 microcoulombs per
kilogram of air (258 µC·kg–1 of
air).
Gray (Gy) Replaces RadGray (Gy) Replaces Rad
In the SI system, the unit of
radiation dose is the gray (Gy),
and 1 Gy =100 rad.
In the SI system, the unit of
radiation dose is the gray (Gy),
and 1 Gy =100 rad.
Sievert (Sv) Replaces RemSievert (Sv) Replaces Rem
In the SI system, the unit of
radiation absorbed by the human
body is Sievert (Sv), and
1 Sv = 100 rem.
In the SI system, the unit of
radiation absorbed by the human
body is Sievert (Sv), and
1 Sv = 100 rem.
Maximum Permissible DoseMaximum Permissible Dose
1. Permissible dose is defined by
the NIST as the dose of radiation
that is not expected to cause
appreciable bodily injury to a
person.
1. Permissible dose is defined by
the NIST as the dose of radiation
that is not expected to cause
appreciable bodily injury to a
person.
Maximum Permissible DoseMaximum Permissible Dose
2. The following restrictions for the
maximum annual permissible
dose limits for classified workers
should be observed:
a. Total effective dose
equivalent being equal to
5 rem (0.05 Sv).
2. The following restrictions for the
maximum annual permissible
dose limits for classified workers
should be observed:
a. Total effective dose
equivalent being equal to
5 rem (0.05 Sv).
Maximum Permissible DoseMaximum Permissible Dose
Or
b. The sum of the absorbed dose
to any individual organ or tissue
other than the lens of the eye
being maximum equal to
50 rem (0.5 Sv).
Or
b. The sum of the absorbed dose
to any individual organ or tissue
other than the lens of the eye
being maximum equal to
50 rem (0.5 Sv).
Maximum Permissible DoseMaximum Permissible Dose
c. The dose absorbed by lens of the
eye be maximum of 15 rem (0.15
Sv).
d. A shallow dose equivalent of
50 rem (0.5 Sv) to the skin of the
whole body or to the skin of any
extremity.
c. The dose absorbed by lens of the
eye be maximum of 15 rem (0.15
Sv).
d. A shallow dose equivalent of
50 rem (0.5 Sv) to the skin of the
whole body or to the skin of any
extremity.
Maximum Permissible DoseMaximum Permissible Dose
3. The maximum annual radiation
dose is limited to 5 rem (0.05 Sv).
4. The absorbed dose shouldn’t
exceed 0.5 rem (5 mSv) during an
entire pregnancy.
3. The maximum annual radiation
dose is limited to 5 rem (0.05 Sv).
4. The absorbed dose shouldn’t
exceed 0.5 rem (5 mSv) during an
entire pregnancy.
Maximum Permissible DoseMaximum Permissible Dose
5. Dose limits to the general public
shall not exceed 0.002 rem or
2 mrem (0.02 mSv) per hour or
exceed 0.5 rem or 500 mrem
(5 mSv) annually.
5. Dose limits to the general public
shall not exceed 0.002 rem or
2 mrem (0.02 mSv) per hour or
exceed 0.5 rem or 500 mrem
(5 mSv) annually.
Protection Against RadiationProtection Against Radiation
Safe radiographic techniques and
radiographic installation design
are achievable by applying these
principles:
1. Time: Keep the time close
to a radiation source as low as
possible.
Safe radiographic techniques and
radiographic installation design
are achievable by applying these
principles:
1. Time: Keep the time close
to a radiation source as low as
possible.
Protection Against RadiationProtection Against Radiation
2. Distance: Keep the distance
from a radiation source a high as
possible.
3. Shielding: Keep adequate
shielding for radiation source.
2. Distance: Keep the distance
from a radiation source a high as
possible.
3. Shielding: Keep adequate
shielding for radiation source.
Allowable Working TimeAllowable Working Time
1. The amount of absorbed radiation
by the human body is directly
proportional to the time that the
body is exposed to radiation.
Example: 2 rem (0.2 mSv) in
60 s = 10 mrem (1 mSv) in 5 min.
1. The amount of absorbed radiation
by the human body is directly
proportional to the time that the
body is exposed to radiation.
Example: 2 rem (0.2 mSv) in
60 s = 10 mrem (1 mSv) in 5 min.
Allowable Working TimeAllowable Working Time
2. Allowable working time for working with
gamma sources is calculated by
measuring radiation intensity and
substituting it in the following equation:
allowable working time in hr/week =
permissible exposure in Ci/wk /
exposure rate in Ci/h
2. Allowable working time for working with
gamma sources is calculated by
measuring radiation intensity and
substituting it in the following equation:
allowable working time in hr/week =
permissible exposure in Ci/wk /
exposure rate in Ci/h
Working DistanceWorking Distance
1. The greater the distance from a
radiation source, the lower the
radiation intensity.
2. The inverse square law is used
is used to calculate radiation
intensities at various distances
from a radiation source.
1. The greater the distance from a
radiation source, the lower the
radiation intensity.
2. The inverse square law is used
is used to calculate radiation
intensities at various distances
from a radiation source.
Working DistanceWorking Distance
I1/I2 = D22/D2
1
where I1 and I2 are intensities at
distances D1 and aD2,
respectively.
I1/I2 = D22/D2
1
where I1 and I2 are intensities at
distances D1 and aD2,
respectively.
Working DistanceWorking Distance
3. The same principles hold for X-radiation. The intensity at a known distance with predetermined current and voltage setting (usually given by the X-ray tubes manufacturers) can be determined by applying the inverse square law.
3. The same principles hold for X-radiation. The intensity at a known distance with predetermined current and voltage setting (usually given by the X-ray tubes manufacturers) can be determined by applying the inverse square law.
Working DistanceWorking Distance
4. Radiation intensity at any point is
the sum of the primary radiation
and the secondary (scattered)
radiation at that point.
4. Radiation intensity at any point is
the sum of the primary radiation
and the secondary (scattered)
radiation at that point.
ShieldingShielding
1. Materials commonly used for
shielding to reduce personnel
exposures are lead, steel, water and
concrete.
1. Materials commonly used for
shielding to reduce personnel
exposures are lead, steel, water and
concrete.
ShieldingShielding
2. Shielding cannot stop all of the
energy of X-radiation or gamma
radiation; therefore, it is practical to
measure shielding efficiency in
terms of half value layers.
2. Shielding cannot stop all of the
energy of X-radiation or gamma
radiation; therefore, it is practical to
measure shielding efficiency in
terms of half value layers.
ShieldingShielding
3. Half value layer (HVL) is that
amount of shielding that will stop
half of the radiation of a given
intensity.
3. Half value layer (HVL) is that
amount of shielding that will stop
half of the radiation of a given
intensity.
ShieldingShielding
4. Similarly, shielding efficiency is often measured in tenth value layers. A tenth value layer is that amount of shielding that will stop nine tenth of the radiation of a given intensity. (See the following tables.)
4. Similarly, shielding efficiency is often measured in tenth value layers. A tenth value layer is that amount of shielding that will stop nine tenth of the radiation of a given intensity. (See the following tables.)
X-ray half value layersX-ray half value layers
Gamma ray half and tenth value layers
Gamma ray half and tenth value layers
Exposure AreaExposure Area
1. Exposure areas should consist of a
room with concrete or block walls,
lined with lead or other suitable
shielding materials.
2. Exposure area can be an enclosed
shielding cabinet large enough for
the test objects and with reliable
safety features.
1. Exposure areas should consist of a
room with concrete or block walls,
lined with lead or other suitable
shielding materials.
2. Exposure area can be an enclosed
shielding cabinet large enough for
the test objects and with reliable
safety features.
Exposure AreaExposure Area
3. Controls should be located outside the exposure area.
4. In field radiography or temporary job sites, safe distance in relation to exposure must be determined and be secured by:
a. Guard rails or ropes.
b. Legible radiation warning signs.
c. Sufficient shielding.
3. Controls should be located outside the exposure area.
4. In field radiography or temporary job sites, safe distance in relation to exposure must be determined and be secured by:
a. Guard rails or ropes.
b. Legible radiation warning signs.
c. Sufficient shielding.
Exposure AreaExposure Area
5. Only monitored radiographers are
permitted in the radiation area.
6. Keeping a safe distance from the
radiation source is the simplest and
most effective safety consideration
in field radiography.
5. Only monitored radiographers are
permitted in the radiation area.
6. Keeping a safe distance from the
radiation source is the simplest and
most effective safety consideration
in field radiography.
Radiation Protective ConstructionRadiation Protective Construction
1. Lead and concrete are the most
common materials used to protect
against radiation.
2. Shielding measurements are
usually expressed in terms of
thickness.
1. Lead and concrete are the most
common materials used to protect
against radiation.
2. Shielding measurements are
usually expressed in terms of
thickness.
Radiation Protective ConstructionRadiation Protective Construction
3. Ensuring a leak-proof shielding is
very important.
4. Sheets of lead must be overlapped,
and nails and screws in the walls
must be covered with adequate
leads.
3. Ensuring a leak-proof shielding is
very important.
4. Sheets of lead must be overlapped,
and nails and screws in the walls
must be covered with adequate
leads.
Radiation Protective ConstructionRadiation Protective Construction
5. Pipes, conduits and air ducts
passing through the walls of the
shielding must be completely
shielded (see the following
figure).
5. Pipes, conduits and air ducts
passing through the walls of the
shielding must be completely
shielded (see the following
figure).
Radiation Protective ConstructionRadiation Protective Construction
6. The thickness of lead is dependent on two factors:
a. Energy of the radiation source.
b. Occupancy of the surrounding areas.
7. Other than lead, structural materials such as concrete and brick are often used as shielding materials.
6. The thickness of lead is dependent on two factors:
a. Energy of the radiation source.
b. Occupancy of the surrounding areas.
7. Other than lead, structural materials such as concrete and brick are often used as shielding materials.
Radiation Protective ConstructionRadiation Protective Construction
8. At voltages greater than 400 kV,
concrete is used as shielding
because:
a. Difficulty installing very thick lead.
b. Thick sheets of lead are cost-
prohibitive.
8. At voltages greater than 400 kV,
concrete is used as shielding
because:
a. Difficulty installing very thick lead.
b. Thick sheets of lead are cost-
prohibitive.
Radiation Protective ConstructionRadiation Protective Construction
c. Concrete is the best alternative
material because of its radiation
protection property and its
construction simplicity.
c. Concrete is the best alternative
material because of its radiation
protection property and its
construction simplicity.
Gamma Ray RequirementsGamma Ray Requirements
1. Special radiation protection is required for gamma radiation based on two factors:
a. Gamma radiation cannot be shot off.
b. Gamma radiation has considerable penetrating ability.
1. Special radiation protection is required for gamma radiation based on two factors:
a. Gamma radiation cannot be shot off.
b. Gamma radiation has considerable penetrating ability.
Gamma Ray RequirementsGamma Ray Requirements
2. A combination of shielding and
distance is usually used during
gamma radiography.
3. Specially labeled storage
containers are necessary to
store gamma sources when not
in use.
2. A combination of shielding and
distance is usually used during
gamma radiography.
3. Specially labeled storage
containers are necessary to
store gamma sources when not
in use.
Gamma Ray RequirementsGamma Ray Requirements
4. After every use, readings with survey
meters are taken to ensure the source is
safely stored.
5. Special projectors (called pigs) or
isotope cameras containing heavy
shielding made of lead or depleted
uranium should be used for using
radioisotope sources.
4. After every use, readings with survey
meters are taken to ensure the source is
safely stored.
5. Special projectors (called pigs) or
isotope cameras containing heavy
shielding made of lead or depleted
uranium should be used for using
radioisotope sources.
United States Nuclear Regulatory CommissionUnited States Nuclear
Regulatory Commission
1. The NRC regulates handling, storage and use of radioisotopes.
2. Figures 5.2 and 5.3 in the Radiographic Testing Classroom Training Book show NRC Form-4 and NRC Form-5, used to monitor the occupational dose history.
1. The NRC regulates handling, storage and use of radioisotopes.
2. Figures 5.2 and 5.3 in the Radiographic Testing Classroom Training Book show NRC Form-4 and NRC Form-5, used to monitor the occupational dose history.
Occupational Radiation Exposure Limits
Occupational Radiation Exposure Limits
1. Limitations on individual dosage
greater than those listed in the
following table may be permitted with
the following conditions:
a. The dose for the whole body
does not exceed 5 rem (0.05
Sv) during any calendar year.
1. Limitations on individual dosage
greater than those listed in the
following table may be permitted with
the following conditions:
a. The dose for the whole body
does not exceed 5 rem (0.05
Sv) during any calendar year.
Occupational Radiation Exposure Limits
Occupational Radiation Exposure Limits
b. The individual’s accumulated
occupational dose has been
recoded on NRC Form-4 and the
individual has signed the form.
b. The individual’s accumulated
occupational dose has been
recoded on NRC Form-4 and the
individual has signed the form.
Maximum permissible doseMaximum permissible dose
Levels of Radiation in Unrestricted Areas
Levels of Radiation in Unrestricted Areas
The following image shows the
exposure limits in an unrestricted
area.
The following image shows the
exposure limits in an unrestricted
area.
Personnel MonitoringPersonnel Monitoring
There are different personnel
monitoring devices required for use
by radiographers and their assistants
during radiographic operations:
There are different personnel
monitoring devices required for use
by radiographers and their assistants
during radiographic operations:
Personnel MonitoringPersonnel Monitoring
1. Film badges.
2. Thermoluminescent dosimeters
(TLDs).
3. Optically stimulated
luminescence badges (OSL).
1. Film badges.
2. Thermoluminescent dosimeters
(TLDs).
3. Optically stimulated
luminescence badges (OSL).
Personnel MonitoringPersonnel Monitoring
4. Direct reading dosimeters.
5. Pocket dosimeters.
6. Electronic personal dosimeters.
The last two types should be
capable of measuring exposures
from 0 to 200 mR (0 to 2 mSv).
4. Direct reading dosimeters.
5. Pocket dosimeters.
6. Electronic personal dosimeters.
The last two types should be
capable of measuring exposures
from 0 to 200 mR (0 to 2 mSv).
Caution Signs, Labels and SignalsCaution Signs, Labels and Signals
1. The radiation symbol should be placed in:
a. Exposure areas.
b. Containers for transporting and storing radioactive
materials.
2. The words caution or danger must appear.
1. The radiation symbol should be placed in:
a. Exposure areas.
b. Containers for transporting and storing radioactive
materials.
2. The words caution or danger must appear.
Caution Signs, Labels and SignalsCaution Signs, Labels and Signals
3. The words radioactive material
should be marked on containers of
radioactive materials and the areas
housing such containers.
3. The words radioactive material
should be marked on containers of
radioactive materials and the areas
housing such containers.
Caution Signs, Labels and SignalsCaution Signs, Labels and Signals
4. Exposure devices should have a radiation symbol and the phrase, Danger radioactive material – do not handle. Company information and a 24 h phone number must be mentioned on the sign.
4. Exposure devices should have a radiation symbol and the phrase, Danger radioactive material – do not handle. Company information and a 24 h phone number must be mentioned on the sign.
Exposure Devices and Storage Containers
Exposure Devices and Storage Containers
Based on the radiation regulations:
1. Exposure devices must have the name
of the company or laboratory and the
location of the office placed in a
noticeable site on the device.
2. All of the labels, signs, etc. shall be
legible.
Based on the radiation regulations:
1. Exposure devices must have the name
of the company or laboratory and the
location of the office placed in a
noticeable site on the device.
2. All of the labels, signs, etc. shall be
legible.
Radiation Survey Instrumentation Requirements
Radiation Survey Instrumentation Requirements
1. Radiographers should have operable
and calibrated radiation survey meters.
2. Each exposure device shall be
accompanied by a survey meter.
3. The meters shall have a range of
2 mR (0.02 mSv) per hour through
1 R (0.1 Sv) per hour.
1. Radiographers should have operable
and calibrated radiation survey meters.
2. Each exposure device shall be
accompanied by a survey meter.
3. The meters shall have a range of
2 mR (0.02 mSv) per hour through
1 R (0.1 Sv) per hour.
Radiation Surveys Radiation Surveys
1. An operable and calibrated radiation
survey instrumentation should be
available at an exposure area.
1. An operable and calibrated radiation
survey instrumentation should be
available at an exposure area.
Radiation SurveysRadiation Surveys
2. When working with radioisotopes, a
radioactive survey shall be made
around the camera to ensure the
source has been returned to its
shielded condition. This is known
as 360º sweep.
2. When working with radioisotopes, a
radioactive survey shall be made
around the camera to ensure the
source has been returned to its
shielded condition. This is known
as 360º sweep.
Radiation Surveys Radiation Surveys
3. Before storing each sealed source,
a radiation survey shall be made to
be sure that the source is in its
shielded position.
4. All these readings shall be recorded
on a radiation report survey.
3. Before storing each sealed source,
a radiation survey shall be made to
be sure that the source is in its
shielded position.
4. All these readings shall be recorded
on a radiation report survey.
Detection and Measurement Instruments
Detection and Measurement Instruments
There are different instruments that
measure the radiation based on the
ionization produced in a gas. These
instruments fall into two categories:
1. Instruments that measure total dose
exposure.
2. Instruments that measure dose rate (radiation intensity).
There are different instruments that
measure the radiation based on the
ionization produced in a gas. These
instruments fall into two categories:
1. Instruments that measure total dose
exposure.
2. Instruments that measure dose rate (radiation intensity).
Instruments that Measure Total Dose Exposure
Instruments that Measure Total Dose Exposure
a. Pocket dosimeter.
b. Electronic personnel dosimeters.
c. Thermoluminescent dosimeters
(TLDs).
d. Optically stimulated
luminescence (OSL) badges.
a. Pocket dosimeter.
b. Electronic personnel dosimeters.
c. Thermoluminescent dosimeters
(TLDs).
d. Optically stimulated
luminescence (OSL) badges.
Instruments that Measure Dose Rate
Instruments that Measure Dose Rate
Instruments that measure dose rate are called survey meters.
a. Ionization chambers.
b. Geiger-mueller counters.
Instruments that measure dose rate are called survey meters.
a. Ionization chambers.
b. Geiger-mueller counters.
Pocket DosimetersPocket Dosimeters
1. The pocket dosimeter is a small
device, about the size of a
fountain pen, as shown in the
following picture.
1. The pocket dosimeter is a small
device, about the size of a
fountain pen, as shown in the
following picture.
Pocket DosimetersPocket Dosimeters
1. Its operation is based on two
main principles:
a. Radiation causes
ionization
in a gas.
b. Similar electrical changes
repel each other.
1. Its operation is based on two
main principles:
a. Radiation causes
ionization
in a gas.
b. Similar electrical changes
repel each other.
Pocket DosimetersPocket Dosimeters
2. The dosimeter should be
properly charged (the indicator
on zero scale) before using.
2. The dosimeter should be
properly charged (the indicator
on zero scale) before using.
Pocket DosimetersPocket Dosimeters
3. Pocket dosimeters are designed
with a sensitivity that permits them
to be scaled in doses from 0 to 200
mR (0 to 2 mSv).
4. Pocket dosimeters must be
calibrated annually, per NRC
regulation, and the date should be
labeled on them.
3. Pocket dosimeters are designed
with a sensitivity that permits them
to be scaled in doses from 0 to 200
mR (0 to 2 mSv).
4. Pocket dosimeters must be
calibrated annually, per NRC
regulation, and the date should be
labeled on them.
Personal Electronic DosimetersPersonal Electronic Dosimeters
1. Personal electronic dosimeters (or electronic dosimeters) have different features:
a. Easy to use.
b. Sensitive.
c. Different dosimeter functions can be enabled or disabled.
1. Personal electronic dosimeters (or electronic dosimeters) have different features:
a. Easy to use.
b. Sensitive.
c. Different dosimeter functions can be enabled or disabled.
Personal Electronic DosimetersPersonal Electronic Dosimeters
2. The electronic dosimeter provides dose, dose rate and set point check, and usually operates with an AA battery.
3. The set points can be present to definitive alarm points.
4. The pocket size monitors provide three-digit digital display.
2. The electronic dosimeter provides dose, dose rate and set point check, and usually operates with an AA battery.
3. The set points can be present to definitive alarm points.
4. The pocket size monitors provide three-digit digital display.
Personal Electronic DosimetersPersonal Electronic Dosimeters
5. The energy response of the pocket sized monitor for gamma and X-ray is 40 keV to 1.2 MeV.
6. They should be calibrated annually.
5. The energy response of the pocket sized monitor for gamma and X-ray is 40 keV to 1.2 MeV.
6. They should be calibrated annually.
Film Badges and Thermoluminescent Dosimeters
Film Badges and Thermoluminescent Dosimeters
1. The film badge (shown on the
next slide), consists of a small
film holder equipped with thin
lead on cadmium filters.
2. The badge is designed only to
be worn by an individual when
working in a radiation area.
1. The film badge (shown on the
next slide), consists of a small
film holder equipped with thin
lead on cadmium filters.
2. The badge is designed only to
be worn by an individual when
working in a radiation area.
Optically Stimulated Luminescence (OSL) Badge
Optically Stimulated Luminescence (OSL) Badge
1. OSL badges measure beta (b),
gamma, neutron and
X-radiation exposures.
2. The OSL is a thin strip of
specially formulated aluminum
oxide crystalline material.
1. OSL badges measure beta (b),
gamma, neutron and
X-radiation exposures.
2. The OSL is a thin strip of
specially formulated aluminum
oxide crystalline material.
Optically Stimulated Luminescence (OSL) Badge
Optically Stimulated Luminescence (OSL) Badge
3. It detects energies from 5 keV to
40 MeV for photons, 150 keV to
10 MeV for beta particles, and 40
keV to 35 MeV for neutrons.
4. The dose measurements range
from 1 mrem to 1000 rem.
3. It detects energies from 5 keV to
40 MeV for photons, 150 keV to
10 MeV for beta particles, and 40
keV to 35 MeV for neutrons.
4. The dose measurements range
from 1 mrem to 1000 rem.
Ionization Chamber InstrumentsIonization Chamber Instruments
1. Ionization chamber instruments
measure the radiation intensity
(dose rate) in milliroentgen per hour
or millisievert per hour.
2. Ionization chamber instruments
typically attain an accuracy of
±15%, except in low intensity
radiation areas.
1. Ionization chamber instruments
measure the radiation intensity
(dose rate) in milliroentgen per hour
or millisievert per hour.
2. Ionization chamber instruments
typically attain an accuracy of
±15%, except in low intensity
radiation areas.
Ionization Chamber InstrumentsIonization Chamber Instruments
3. Radiation intensity measurements
in areas of low intensity radiation
are usually made with geiger-
mueller counters.
4. Ionization chamber instruments
should be calibrated annually.
3. Radiation intensity measurements
in areas of low intensity radiation
are usually made with geiger-
mueller counters.
4. Ionization chamber instruments
should be calibrated annually.
Geiger-Mueller CountersGeiger-Mueller Counters
1. A geiger-mueller counter is a high sensitive radiation detection device.
2. Geiger-mueller counters are typically accurate to ±20% for the quantity of radiation to which they are calibrated.
3. They should be calibrated annually.
1. A geiger-mueller counter is a high sensitive radiation detection device.
2. Geiger-mueller counters are typically accurate to ±20% for the quantity of radiation to which they are calibrated.
3. They should be calibrated annually.
Area Alarm SystemsArea Alarm Systems
2. These systems consist of one or
more sensing elements usually
ionization chambers whose
output is fed a central alarm
meter.
2. These systems consist of one or
more sensing elements usually
ionization chambers whose
output is fed a central alarm
meter.
Area Alarm SystemsArea Alarm Systems
3. The meter can be present so that
an audible alarm is sounded,
and a visual indication is given
where permissible radiation
levels are exceeded.
3. The meter can be present so that
an audible alarm is sounded,
and a visual indication is given
where permissible radiation
levels are exceeded.
Electrical SafetyElectrical Safety
1. Because X-ray machines use high
voltage circuits, the radiographer
must comply with safe electrical
procedures.
2. This is more serious specifically for
portable X-ray equipment, which
requires certain electrical
precautions.
1. Because X-ray machines use high
voltage circuits, the radiographer
must comply with safe electrical
procedures.
2. This is more serious specifically for
portable X-ray equipment, which
requires certain electrical
precautions.
Electrical SafetyElectrical Safety
3. During operation or service of
X-ray equipment, the following
precautions, applicable to both
permanent and portable
installations, should be observed
carefully.
3. During operation or service of
X-ray equipment, the following
precautions, applicable to both
permanent and portable
installations, should be observed
carefully.
Electrical SafetyElectrical Safety
a. Do not turn power on until set up
for exposure is completed.
b. Ensure that grounding
instructions are complied with.
a. Do not turn power on until set up
for exposure is completed.
b. Ensure that grounding
instructions are complied with.
Electrical SafetyElectrical Safety
c. Regularly check power cables for signs of
wear, and replace them where
necessary.
d. Avoid handling power cables when
the power is on. The machine’s
operational key should be removed when
not in use.
c. Regularly check power cables for signs of
wear, and replace them where
necessary.
d. Avoid handling power cables when
the power is on. The machine’s
operational key should be removed when
not in use.
Electrical SafetyElectrical Safety
e. If power cables must be handled
with the power on, use safety
equipment such as rubber gloves,
rubber mats and insulated high
voltage sticks.
f. Be sure that water and moisture is not
in close contact with power cables.
e. If power cables must be handled
with the power on, use safety
equipment such as rubber gloves,
rubber mats and insulated high
voltage sticks.
f. Be sure that water and moisture is not
in close contact with power cables.
Electrical SafetyElectrical Safety
g. Ensure that capacitors are
completely discharged before
checking an electronic circuit.
g. Ensure that capacitors are
completely discharged before
checking an electronic circuit.