Standard Test Method for Determining Protection Provided By X-ray Shielding Garments Used in Medical X-ray Fluoroscopy from Sources of Scattered X-Rays

SIGNIFICANCE AND USE
5.1 This test method is designed to provide a standardized procedure to ensure comparable results between manufacturers, testing laboratories, and users.  
5.2 This test method attempts to realistically quantify the radiation protection provided by radiation protective garments under real-world conditions for workers primarily exposed to scattered radiation in medical fluoroscopy work.  
5.3 This test method is designed to simulate exposure conditions to radiation scattered from the body of the patient undergoing fluoroscopy through an angle of 90° from the primary X-ray beam.  
5.4 The test method is designed to include contributions of radiation dose to the wearer from secondary radiation emitted from the shielding material.
SCOPE
1.1 This test method establishes a procedure for measuring the relative reduction in the intensity of X-radiation provided by shielding garments to the human user under conditions simulating actual use.  
1.2 This test method provides a condition simulating X-rays generated between 60 and 130 kV that are scattered through an angle of 90° by a water equivalent material.  
1.3 This test method applies to both leaded and no-leaded radiation protective materials.  
1.4 This test method provides a method for inclusion of secondary radiations generated within the protective material into a more realistic evaluation of radiation protection.  
1.5 The values given in SI units are to be regarded as standard. No other units of measurement are included in this standard.  
1.6 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety, health, and environmental practices and determine the applicability of regulatory limitations prior to use. Some specific hazards statements are given in Section 7.  
1.7 This international standard was developed in accordance with internationally recognized principles on standardization established in the Decision on Principles for the Development of International Standards, Guides and Recommendations issued by the World Trade Organization Technical Barriers to Trade (TBT) Committee.

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Publication Date
30-Nov-2022
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ASTM F3094-14(2022) - Standard Test Method for Determining Protection Provided By X-ray Shielding Garments Used in Medical X-ray Fluoroscopy from Sources of Scattered X-Rays
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This international standard was developed in accordance with internationally recognized principles on standardization established in the Decision on Principles for the
Development of International Standards, Guides and Recommendations issued by the World Trade Organization Technical Barriers to Trade (TBT) Committee.
Designation: F3094 − 14 (Reapproved 2022)
Standard Test Method for
Determining Protection Provided By X-ray Shielding
Garments Used in Medical X-ray Fluoroscopy from Sources
of Scattered X-Rays
This standard is issued under the fixed designation F3094; the number immediately following the designation indicates the year of
original adoption or, in the case of revision, the year of last revision.Anumber in parentheses indicates the year of last reapproval.A
superscript epsilon (´) indicates an editorial change since the last revision or reapproval.
1. Scope 2. Referenced Documents
1.1 This test method establishes a procedure for measuring 2.1 ASTM Standards:
the relative reduction in the intensity of X-radiation provided F1494Terminology Relating to Protective Clothing
by shielding garments to the human user under conditions F2547Test Method for Determining the Attenuation Prop-
simulating actual use. erties in a Primary X-ray Beam of Materials Used to
Protect Against Radiation Generated During the Use of
1.2 ThistestmethodprovidesaconditionsimulatingX-rays
X-ray Equipment
generatedbetween60and130kVthatarescatteredthroughan
2.2 IEC Standard:
angle of 90° by a water equivalent material.
IEC 61331-1 Ed. 2.0Protective DevicesAgainst Diagnostic
1.3 This test method applies to both leaded and no-leaded
Medical X-radiation: Part 1—Determination of Attenua-
radiation protective materials.
tion Properties of Materials
1.4 This test method provides a method for inclusion of
3. Terminology
secondary radiations generated within the protective material
into a more realistic evaluation of radiation protection. 3.1 Definitions:
3.1.1 attenuation, n—for radiological protective material,
1.5 The values given in SI units are to be regarded as
the fractional reduction in the intensity of the X-ray beam
standard. No other units of measurement are included in this
resultingfromtheinteractionsbetweentheX-raybeamandthe
standard.
protective material when the X-ray beam passes through the
1.6 This standard does not purport to address all of the
protective material.
safety concerns, if any, associated with its use. It is the
3.1.1.1 Discussion—Itisimportanttonotethatthemeasure-
responsibility of the user of this standard to establish appro-
ment of attenuation (as specified by Test Method F2547)
priate safety, health, and environmental practices and deter-
specifically excludes the contribution of secondary radiation
mine the applicability of regulatory limitations prior to use.
from the measurement. The present standard provides a
Some specific hazards statements are given in Section 7.
method for incorporating those contributions of radiation dose
1.7 This international standard was developed in accor-
to the wearer of protective garments. (See 3.1.10.)
dance with internationally recognized principles on standard-
3.1.2 coeffıcient of variation—the ratio of the standard
ization established in the Decision on Principles for the
deviation of a sample to the sample mean.
Development of International Standards, Guides and Recom-
3.1.3 exposure, n—for radiological purposes the amount of
mendations issued by the World Trade Organization Technical
ionization charge of one sign produced in a defined volume of
Barriers to Trade (TBT) Committee.
dry air at standard temperature and pressure, caused by
1 2
ThistestmethodisunderthejurisdictionofASTMCommitteeF23onPersonal For referenced ASTM standards, visit the ASTM website, www.astm.org, or
ProtectiveClothingandEquipmentandisthedirectresponsibilityofSubcommittee contact ASTM Customer Service at service@astm.org. For Annual Book of ASTM
F23.70 on Radiological Hazards. Standards volume information, refer to the standard’s Document Summary page on
Current edition approved Dec. 1, 2022. Published December 2022. Originally the ASTM website.
approved in 2014. Last previous edition approved in 2014 as F3094–14. DOI: Available from International Electrotechnical Commission (IEC), 3, rue de
10.1520/F3094-14R22. Varembé, P.O. Box 131, CH-1211 Geneva 20, Switzerland, http://www.iec.ch.
Copyright © ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States
F3094 − 14 (2022)
interaction with X-rays. Exposure is expressed in units of 3.1.10 protection rating, n—forthepurposesofradiological
coulombs/kg of air in SI units. An older unit called the protectioninthistestmethod,thepercentageofexposureatthe
–4
Roentgen (R) is also used, where1R= 2.58 × 10 C/kg. skin surface of the wearer of the protective garment relative to
the exposure on that surface in the absence of the protective
3.1.4 fluorescent radiation, n—a form of secondary radia-
garment, measured under scatter equivalent conditions for a
tion following photoelectric collisions between X-rays and
particular radiation quality.
orbital electrons of heavier elements such as those used in
protectivematerials,whereuponelectronrearrangementsatthe
3.1.11 scatter equivalent conditions—specific primary
atomic level result in the emission of one or more fluorescent X-ray spectra defined in terms of kV and HVL that simulate
photons.
radiation scattered from a water equivalent medium measured
3.1.4.1 Discussion—Measurements to include fluorescent at 90° to the beam incidence on that medium.
radiation are important because they may contribute to the
3.1.11.1 Discussion—Measuring the actual degree of pro-
radiation exposure to the wearer of radiation protective gar-
tection from scattered X-rays provided by radiation protective
ments.
garments under real-world conditions is technically difficult
and subject to large uncertainties.Actual scatter intensities are
3.1.5 half-value layer (HV), n—thethicknessof99.9%pure
too low and measurements have excessively high uncertainties
aluminum in millimetres (commonly designated mm Al) that
when evaluated in practical conditions. The scatter equivalent
reducestheintensityofanX-raybeambyonehalfofitsinitial
conditionsdescribeconditionsthatconservativelyapproximate
value.
the energies of 90° scatter produced when a water medium
3.1.5.1 Discussion—HVL is commonly used to designate
(body of a human or animal) is exposed toTest Method F2547
the penetrating ability of an X-ray beam containing many
beam qualities. Use of the surrogate primary beams provides
X-ray energies (as is the case with standard X-ray sources).A
conditions that are practical to test under field conditions.
highervalueofAlinmmAlwouldindicateamorepenetrating
X-ray beam. Note that HVLmay also be specified in materials
3.1.12 scatter radiation, n—a form of secondary radiation
other than Al, although only Al is used in this document.
where X-radiation is deflected to a changed direction with or
without a loss in energy by collisions between X-ray photons
3.1.6 ionization chamber—a device that measures the elec-
and orbital electrons of atoms in the path of the X-rays;
tricalchargeliberatedduringtheionizationofairmoleculesby
scattering events in medical procedures mainly occur with loss
electromagnetic radiation (X-rays for the purposes of this test
of energy due to the Compton Effect such that the average
method), expressed in units of coulombs per kg of air.
energies of scattered X-rays are less than those of the direct
3.1.6.1 Discussion—The measurement of exposure is de-
primary beam.
fined for an air ionization chamber. The chamber used in this
method must be of a flat, parallel-plate design.
3.1.13 secondary radiation, n—radiation that is produced in
a material by scattering or emission when the material is
3.1.7 kilovolts, or kilovolts peak (kV or kVp), n—for the
exposed to a source of X-rays.
purposes of radiological protection, the maximum electrical
potential across an X-ray tube during exposure. 3.1.13.1 Discussion—Secondary radiation is of importance
because: (1) the hazard to medical X-ray fluoroscopy workers
3.1.7.1 Discussion—The kV or kVp determines the maxi-
mum photon energy in kilo-electron volts (keV) of an X-ray is principally from X-rays scattered from the patient and other
materials within the primary X-ray beam, and (2) fluorescent
beam; standard X-ray beams contain many photon energies
radiation produced within the protective material can contrib-
most of which are less than this maximum value.
ute to the radiation exposure to the wearer of the radiation
3.1.8 lead equivalency—for radiological protective material
protective garments.
the thickness in millimetres (commonly designated mm Pb) of
greaterthan99.9%puritythatprovidesthesameattenuationas 3.1.14 standard sample dimensions—test samples and lead
standardscuttoanareasuitedtothemeasurementsetupinFig.
a given protective material.
3.1.8.1 Discussion—Radiationprotectivematerialsarecom- 1, ideally by using a template.
monly made with little or no lead, thus lead equivalence will 3.1.14.1 Discussion—It may be desired to test finished
vary with X-ray energy and with the composition of the
protective clothing that are not cut to standard sample dimen-
protective material. Lead equivalence should be specified at a sionsusingthistestmethod.Thismaybedone,butmayrequire
specific energy. This test method specifies a method for
a special test jig to support the material in proper orientation
determining the attenuation in pure lead materials but does not andconfigurationtomeetthistestmethod.Suchaprocedureis
require a specific lead equivalence. If lead equivalence is not described in this test method.
specified, it should be specified at a single scatter equivalent
3.1.15 wave form ripple, n—for radiological purposes, the
condition.
peak-to-peak variation in the voltage potential applied to the
3.1.9 primary X-rays, n—the X-rays emitted from the target
X-raytubeduringexposure.Greatervoltageripple(commonin
of an X-ray tube subjected to an accelerating potential suffi-
older X-ray generators) tends to reduce the intensity and
cient to cause X-ray emission.
3.1.9.1 Discussion—Primary X-rays are distinguished from
secondary X-rays emitted from a material exposed to primary
McCaffrey, J. P., Tessier, F., and Shen, H., “Radiation Shielding Materials and
X-rays. Secondary X-rays are generally less penetrating than
RadiationScatterEffectsforInterventionalRadiology(IR)Physicians,” Med. Phys.,
primary X-rays. Vol 39, No. 7, July 2012.
F3094 − 14 (2022)
ments correspond to most common fluoroscopic conditions at
80 kV, a high kV condition for a standard fluoroscope at
100kV, and a condition corresponding to scatter produced
from CT scanning at 130 kV. These scatter equivalent condi-
tions correspond to direct beam measurement at 70, 85, and
105 kV with filtrations adjusted to achieve HVLs of 3.4, 4.0,
and 5.1 mm Al respectively.
5. Significance and Use
5.1 This test method is designed to provide a standardized
procedure to ensure comparable results between
manufacturers, testing laboratories, and users.
5.2 This test method attempts to realistically quantify the
radiation protection provided by radiation protective garments
under real-world conditions for workers primarily exposed to
scattered radiation in medical fluoroscopy work.
1. Diaphragm
5.3 This test method is designed to simulate exposure
2. Beam filtration
conditions to radiation scattered from the body of the patient
3. Diaphragm
undergoing fluoroscopy through an angle of 90° from the
4. Measuring diaphragm
5. Test material
primary X-ray beam.
6. Flat air ionization measuring chamber
1. IEC 61331-1 Ed. 2.0 Protective Devices Against Diagnostic Medical 5.4 The test method is designed to include contributions of
X-radiation, Part 1: Determination of Attenuation Properties.
radiation dose to the wearer from secondary radiation emitted
2. McCaffrey, J. P., Tessier, F., and Shen, H., “Radiation Shielding Materials and
from the shielding material.
Radiation Scatter Effects for Interventional Radiology (IR) Physicians,” Med.
Phys., Vol 39, No. 7, 2012, pp. 4537–4546.
6. Apparatus
FIG. 1 Test Setup
6.1 Primary X-ray Beam Source—A variable power X-ray
generator coupled to a tungsten anode X-ray tube with the
following characteristics:
penetrating ability of the resulting X-ray beam compared to
6.1.1 Wave form ripple cannot exceed 3%, and may not
units with little or no voltage ripple.
employ capacitor discharge methods where the voltage poten-
3.2 Some definitions are reproduced for convenience from
tial falls more than 5% during the test exposure.
Test Method F2547. For definitions of other terms related to
6.2 kV Monitoring—Kilovoltage shall be actively measured
protective clothing used in this test method, refer to Terminol-
during testing with an invasive or non-invasive kV measuring
ogy F1494.
device capable of measuring potential within 0.5 kV of the
4. Summary of Test Method
actual tube.
6.2.1 Thecoefficientofvariationinvoltagepotentialcannot
4.1 A primary X-ray beam with a standardized X-ray
exceed 0.05 in four consecutive exposures using the potential
spectrum and a constant intensity with the conditions listed in
setting(s) for testing.
Table 1 for the scatter equivalent conditions employed to
measure the attenuation in test samples using the inverse
6.3 Exposure Measurement:
broad-beam conditions in Fig. 1.
6.4 An ionization chamber and electrometer capable of
4.2 Attenuation can be measured for scatter equivalent
measuring from 0.258 to 1290 µC/kg (1 mR to 5 R) and
energiescorrespondingtoallprimarybeamenergiesasdefined
calibrated for use with X-rays generated under conditions
by Test Method F2547; however, it is recommended that three
specified by Test Method F2547.
measurements be used in standard reports. These measure-
6.5 The coefficient of variation in exposure cannot exceed
0.05 in four consecutive exposures when measured through
TABLE 1 Standard X-ray Qualities (Columns 1 and 2) and Scatter
4 0.5mm of Pb.
Equivalent Qualities
Direct Beam 90° Scatter Equivalent 6.6 Noise—Detector signal measured under the same con-
kV HVL (mm Al) kV HVL (mm Al)
ditions (integration time) of the measurement but without
60 2.9 50 2.6
X-rays shall not be more than 1% of the minimum measure-
70 3.3 60 2.9
80 4.0 70 3.4 ment recorded through any test material.
90 4.3 75 3.7
6.7 Test Setup—Theapparatusmayuseeitheraverticallyor
100 5.2 85 4.0
110 5.5 90 4.3
horizontally directed X-ray beam provided that the geometry
120 6.3 100 4.5
conforms to that described in Fig. 1.
130 6.7 105 5.1
6.7.1 Beam defining apertures.
F3094 − 14 (2022)
6.7.1.1 Beam apertures designated 1 and 3 in Fig. 1 are 9.2 Measure and document the exposure reproducibility
normally incorporated i
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