ASTM E266-23
(Test Method)Standard Test Method for Measuring Fast-Neutron Reaction Rates by Radioactivation of Aluminum
Standard Test Method for Measuring Fast-Neutron Reaction Rates by Radioactivation of Aluminum
SIGNIFICANCE AND USE
5.1 Refer to Guide E844 for the selection, irradiation, and quality control of neutron dosimeters.
5.2 Refer to Practice E261 for a general discussion of the determination of fast-neutron fluence rate with threshold detectors.
5.3 Pure aluminum in the form of foil or wire is readily available and easily handled. 27Al has an abundance of 100 % (1).3
5.4 24Na has a half-life of 14.958 (2)4 h (2) and emits gamma rays with energies of 1.368630 (5) and 2.754049 (13) MeV (2).
5.5 Fig. 1 shows a plot of the International Reactor Dosimetry and Fusion File (IRDFF-II) cross section (3, 4) versus neutron energy for the fast-neutron reaction 27Al(n,α) 24Na (3) along with a comparison to the current experimental database (5, 6). While the RRDF-2008 and IRDFF-1.05 cross sections extend from threshold up to 60 MeV, due to considerations of the available validation data, the energy region over which this standard recommends use of this cross section for reactor dosimetry applications only extends from threshold at ~4.25 MeV up to 20 MeV. This figure is for illustrative purposes and is used to indicate the range of response of the 27Al(n,α) reaction. Refer to Guide E1018 for recommended sources for the tabulated dosimetry cross sections.
FIG. 1 27Al(n,α)24Na Cross Section, from IRDFF-II Library, with EXFOR Experimental Data
5.6 Two competing activities, 28Al (2.25 (2) minute half-life) and 27Mg (9.458 (12) minute half-life), are formed in the reactions 27Al(n,γ)28Al and 27Al(n,p)27Mg, respectively, but these can be eliminated by waiting 2 h before counting.
SCOPE
1.1 This test method covers procedures measuring reaction rates by the activation reaction 27Al(n,α)24Na.
1.2 This activation reaction is useful for measuring neutrons with energies above approximately 6.5 MeV and for irradiation times up to about two days (for longer irradiations, or when there are significant variations in reactor power during the irradiation, see Practice E261).
1.3 With suitable techniques, fission-neutron fluence rates above 106 cm−2·s−1 can be determined.
1.4 Detailed procedures for other fast neutron detectors are referenced in Practice E261.
1.5 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.
1.6 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.
General Information
- Status
- Published
- Publication Date
- 31-May-2023
- Technical Committee
- E10 - Nuclear Technology and Applications
- Drafting Committee
- E10.05 - Nuclear Radiation Metrology
Relations
- Effective Date
- 01-Apr-2022
- Effective Date
- 01-Mar-2020
- Effective Date
- 01-Mar-2020
- Effective Date
- 01-Oct-2019
- Effective Date
- 01-Jun-2018
- Effective Date
- 01-Oct-2017
- Effective Date
- 01-Oct-2017
- Effective Date
- 01-Jun-2017
- Effective Date
- 01-Oct-2016
- Effective Date
- 15-Feb-2016
- Effective Date
- 01-Sep-2015
- Effective Date
- 01-Jul-2015
- Effective Date
- 01-Jun-2015
- Effective Date
- 15-Mar-2015
- Effective Date
- 15-Oct-2014
Overview
ASTM E266-23 is a detailed standard test method developed by ASTM International for measuring fast-neutron reaction rates by the radioactivation of aluminum. This method utilizes the activation reaction of 27Al(n,α)24Na, providing a precise approach for determining fast-neutron fluence rates, particularly in nuclear reactor environments. Aluminum is selected for its high purity and abundant isotope 27Al, making it ideal for neutron dosimetry and reactor surveillance applications.
The importance of ASTM E266-23 lies in its role in nuclear metrology, dosimetry, and quality assurance for neutron flux measurements. The procedure enables laboratories and nuclear facilities to reliably assess fast-neutron environments, enhancing safety and operational accuracy.
Key Topics
- Activation Reaction: The method utilizes the reaction 27Al(n,α)24Na, which is sensitive to neutrons with energies above approximately 6.5 MeV.
- Detection and Measurement: After irradiating high-purity aluminum, the resulting radioactive 24Na is analyzed via its emitted gamma rays (mainly at 1.37 MeV and 2.75 MeV) using gamma-ray spectrometry.
- Sample Handling: Only highly pure aluminum samples are used to avoid interference from long-lived gamma-emitting impurities. The samples are typically in foil or wire form.
- Irradiation Conditions: The standard is applicable for irradiation periods up to two days and for fission-neutron fluence rates above 1.0 x 10⁶ cm⁻²·s⁻¹.
- Quality Control: Competing activation products, such as 28Al and 27Mg, can be minimized by waiting at least two hours before measuring the radioactivity.
- Cross Section Data: Uses internationally recognized cross-section data libraries (such as IRDFF-II) to ensure accurate dosimetry and comparison with experimental results.
Applications
ASTM E266-23 is crucial in multiple practical settings where precise fast-neutron measurements are necessary:
- Reactor Surveillance: Used to monitor neutron flux and reactions within nuclear power reactors, supporting reactor vessel lifespan assessments and materials performance evaluations.
- Neutron Dosimetry: Enables the calibration and validation of dosimetry systems in both research and operational reactors.
- Calibration Laboratories: Applied by calibration facilities to establish or maintain neutron reference fields.
- Nuclear Safety Programs: Supports safety analyses and regulatory compliance by providing standardized measurement techniques.
- Research & Development: Facilitates fundamental studies in neutron physics, validation of cross sections, and benchmarking of computational reactor models.
- Pressure Vessel Monitoring: Plays a role in the surveillance of pressure vessels by quantifying fast-neutron exposure which can impact material properties over time.
Related Standards
Several ASTM standards are referenced or complement the application of ASTM E266-23, including:
- ASTM E844: Guide for selection and irradiation of neutron dosimeters in reactor surveillance.
- ASTM E261: Practice for determining neutron fluence, fluence rate, and spectra via radioactivation techniques.
- ASTM E181: Guide for calibration and analysis of radionuclides using detector systems.
- ASTM E1005: Test method for application and analysis of radiometric monitors in reactor vessel surveillance.
- ASTM E1018: Guide for application of evaluated cross-section data files in neutron dosimetry.
- ASTM E944: Guide for neutron spectrum adjustment methods.
- ASTM E170 & E456: Terminologies related to radiation measurements, dosimetry, quality, and statistics.
Conclusion
ASTM E266-23 provides a robust and internationally recognized method for measuring fast-neutron reaction rates by radioactivation of aluminum, ensuring accurate neutron dosimetry in nuclear environments. Its emphasis on standardization, cross-section data consistency, and practical sample handling makes it indispensable for reactor surveillance programs, research laboratories, and calibration facilities committed to precision and safety in neutron measurements.
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Frequently Asked Questions
ASTM E266-23 is a standard published by ASTM International. Its full title is "Standard Test Method for Measuring Fast-Neutron Reaction Rates by Radioactivation of Aluminum". This standard covers: SIGNIFICANCE AND USE 5.1 Refer to Guide E844 for the selection, irradiation, and quality control of neutron dosimeters. 5.2 Refer to Practice E261 for a general discussion of the determination of fast-neutron fluence rate with threshold detectors. 5.3 Pure aluminum in the form of foil or wire is readily available and easily handled. 27Al has an abundance of 100 % (1).3 5.4 24Na has a half-life of 14.958 (2)4 h (2) and emits gamma rays with energies of 1.368630 (5) and 2.754049 (13) MeV (2). 5.5 Fig. 1 shows a plot of the International Reactor Dosimetry and Fusion File (IRDFF-II) cross section (3, 4) versus neutron energy for the fast-neutron reaction 27Al(n,α) 24Na (3) along with a comparison to the current experimental database (5, 6). While the RRDF-2008 and IRDFF-1.05 cross sections extend from threshold up to 60 MeV, due to considerations of the available validation data, the energy region over which this standard recommends use of this cross section for reactor dosimetry applications only extends from threshold at ~4.25 MeV up to 20 MeV. This figure is for illustrative purposes and is used to indicate the range of response of the 27Al(n,α) reaction. Refer to Guide E1018 for recommended sources for the tabulated dosimetry cross sections. FIG. 1 27Al(n,α)24Na Cross Section, from IRDFF-II Library, with EXFOR Experimental Data 5.6 Two competing activities, 28Al (2.25 (2) minute half-life) and 27Mg (9.458 (12) minute half-life), are formed in the reactions 27Al(n,γ)28Al and 27Al(n,p)27Mg, respectively, but these can be eliminated by waiting 2 h before counting. SCOPE 1.1 This test method covers procedures measuring reaction rates by the activation reaction 27Al(n,α)24Na. 1.2 This activation reaction is useful for measuring neutrons with energies above approximately 6.5 MeV and for irradiation times up to about two days (for longer irradiations, or when there are significant variations in reactor power during the irradiation, see Practice E261). 1.3 With suitable techniques, fission-neutron fluence rates above 106 cm−2·s−1 can be determined. 1.4 Detailed procedures for other fast neutron detectors are referenced in Practice E261. 1.5 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. 1.6 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.
SIGNIFICANCE AND USE 5.1 Refer to Guide E844 for the selection, irradiation, and quality control of neutron dosimeters. 5.2 Refer to Practice E261 for a general discussion of the determination of fast-neutron fluence rate with threshold detectors. 5.3 Pure aluminum in the form of foil or wire is readily available and easily handled. 27Al has an abundance of 100 % (1).3 5.4 24Na has a half-life of 14.958 (2)4 h (2) and emits gamma rays with energies of 1.368630 (5) and 2.754049 (13) MeV (2). 5.5 Fig. 1 shows a plot of the International Reactor Dosimetry and Fusion File (IRDFF-II) cross section (3, 4) versus neutron energy for the fast-neutron reaction 27Al(n,α) 24Na (3) along with a comparison to the current experimental database (5, 6). While the RRDF-2008 and IRDFF-1.05 cross sections extend from threshold up to 60 MeV, due to considerations of the available validation data, the energy region over which this standard recommends use of this cross section for reactor dosimetry applications only extends from threshold at ~4.25 MeV up to 20 MeV. This figure is for illustrative purposes and is used to indicate the range of response of the 27Al(n,α) reaction. Refer to Guide E1018 for recommended sources for the tabulated dosimetry cross sections. FIG. 1 27Al(n,α)24Na Cross Section, from IRDFF-II Library, with EXFOR Experimental Data 5.6 Two competing activities, 28Al (2.25 (2) minute half-life) and 27Mg (9.458 (12) minute half-life), are formed in the reactions 27Al(n,γ)28Al and 27Al(n,p)27Mg, respectively, but these can be eliminated by waiting 2 h before counting. SCOPE 1.1 This test method covers procedures measuring reaction rates by the activation reaction 27Al(n,α)24Na. 1.2 This activation reaction is useful for measuring neutrons with energies above approximately 6.5 MeV and for irradiation times up to about two days (for longer irradiations, or when there are significant variations in reactor power during the irradiation, see Practice E261). 1.3 With suitable techniques, fission-neutron fluence rates above 106 cm−2·s−1 can be determined. 1.4 Detailed procedures for other fast neutron detectors are referenced in Practice E261. 1.5 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. 1.6 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.
ASTM E266-23 is classified under the following ICS (International Classification for Standards) categories: 17.240 - Radiation measurements; 27.120.30 - Fissile materials and nuclear fuel technology. The ICS classification helps identify the subject area and facilitates finding related standards.
ASTM E266-23 has the following relationships with other standards: It is inter standard links to ASTM E456-13a(2022)e1, ASTM E1018-20, ASTM E1018-20e1, ASTM E944-19, ASTM E844-18, ASTM E456-13A(2017)e1, ASTM E456-13A(2017)e3, ASTM E170-17, ASTM E170-16a, ASTM E170-16, ASTM E170-15a, ASTM E1005-15, ASTM E261-15, ASTM E170-15, ASTM E170-14a. Understanding these relationships helps ensure you are using the most current and applicable version of the standard.
ASTM E266-23 is available in PDF format for immediate download after purchase. The document can be added to your cart and obtained through the secure checkout process. Digital delivery ensures instant access to the complete standard document.
Standards Content (Sample)
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: E266 − 23
Standard Test Method for
Measuring Fast-Neutron Reaction Rates by Radioactivation
of Aluminum
This standard is issued under the fixed designation E266; the number immediately following the designation indicates the year of
original adoption or, in the case of revision, the year of last revision. A number in parentheses indicates the year of last reapproval. A
superscript epsilon (´) indicates an editorial change since the last revision or reapproval.
1. Scope nuclides in Radiation Metrology for Reactor Dosimetry
E261 Practice for Determining Neutron Fluence, Fluence
1.1 This test method covers procedures measuring reaction
27 24 Rate, and Spectra by Radioactivation Techniques
rates by the activation reaction Al(n,α) Na.
E456 Terminology Relating to Quality and Statistics
1.2 This activation reaction is useful for measuring neutrons
E844 Guide for Sensor Set Design and Irradiation for
with energies above approximately 6.5 MeV and for irradiation
Reactor Surveillance
times up to about two days (for longer irradiations, or when
E944 Guide for Application of Neutron Spectrum Adjust-
there are significant variations in reactor power during the
ment Methods in Reactor Surveillance
irradiation, see Practice E261).
E1005 Test Method for Application and Analysis of Radio-
metric Monitors for Reactor Vessel Surveillance
1.3 With suitable techniques, fission-neutron fluence rates
6 −2 −1
above 10 cm ·s can be determined. E1018 Guide for Application of ASTM Evaluated Cross
Section Data File
1.4 Detailed procedures for other fast neutron detectors are
referenced in Practice E261.
3. Terminology
1.5 This standard does not purport to address all of the
3.1 Definitions:
safety concerns, if any, associated with its use. It is the
3.1.1 Refer to Terminologies E170 and E456.
responsibility of the user of this standard to establish appro-
priate safety, health, and environmental practices and deter-
4. Summary of Test Method
mine the applicability of regulatory limitations prior to use.
4.1 High-purity aluminum is irradiated in a neutron field,
1.6 This international standard was developed in accor-
24 27 24
thereby producing radioactive Na from the Al(n,α) Na
dance with internationally recognized principles on standard-
activation reaction.
ization established in the Decision on Principles for the
4.2 The gamma rays emitted by the radioactive decay of
Development of International Standards, Guides and Recom-
Na are counted (see Guide E181) and the reaction rate, as
mendations issued by the World Trade Organization Technical
defined by Practice E261, is calculated from the decay rate and
Barriers to Trade (TBT) Committee.
irradiation conditions.
2. Referenced Documents
4.3 The neutron fluence rate above about 6.5 MeV can then
be calculated from the spectral-weighted neutron activation
2.1 ASTM Standards:
E170 Terminology Relating to Radiation Measurements and cross section as defined by Practice E261.
Dosimetry
5. Significance and Use
E177 Practice for Use of the Terms Precision and Bias in
ASTM Test Methods 5.1 Refer to Guide E844 for the selection, irradiation, and
E181 Guide for Detector Calibration and Analysis of Radio-
quality control of neutron dosimeters.
5.2 Refer to Practice E261 for a general discussion of the
determination of fast-neutron fluence rate with threshold de-
This test method is under the jurisdiction of ASTM Committee E10 on Nuclear
tectors.
Technology and Applications and is the direct responsibility of Subcommittee
E10.05 on Nuclear Radiation Metrology.
5.3 Pure aluminum in the form of foil or wire is readily
Current edition approved June 1, 2023. Published June 2023. Originally
available and easily handled. Al has an abundance of 100 %
approved in 1965. Last previous edition approved in 2017 as E266 – 17. DOI:
(1).
10.1520/E0266-23.
For referenced ASTM standards, visit the ASTM website, www.astm.org, or
contact ASTM Customer Service at service@astm.org. For Annual Book of ASTM
Standards volume information, refer to the standard’s Document Summary page on The boldface numbers in parentheses refer to a list of References at the end of
the ASTM website. this standard.
Copyright © ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States
E266 − 23
24 4 24
5.4 Na has a half-life of 14.958 (2) h (2) and emits spectrograph. If the Na content of the irradiated samples is
gamma rays with energies of 1.368630 (5) and 2.754049 (13) determined from the emission rate of the 2.754049 MeV
MeV (2). gamma ray, the probability of interference from contaminant
gamma rays is much less than if the 1.368630 MeV gamma ray
5.5 Fig. 1 shows a plot of the International Reactor Dosim-
is used.
etry and Fusion File (IRDFF-II) cross section (3, 4) versus
27 24
neutron energy for the fast-neutron reaction Al(n,α) Na (3) 7.2 Encapsulating Materials—Brass, stainless steel, copper,
along with a comparison to the current experimental database
aluminum, quartz, or vanadium have been used as primary
(5, 6). While the RRDF-2008 and IRDFF-1.05 cross sections encapsulating materials. The container should be constructed
extend from threshold up to 60 MeV, due to considerations of
in such a manner that it will not create significant flux
the available validation data, the energy region over which this perturbation and that it may be opened easily, especially if the
standard recommends use of this cross section for reactor
capsule is to be opened remotely (see Guide E844).
dosimetry applications only extends from threshold at ~4.25
MeV up to 20 MeV. This figure is for illustrative purposes and
8. Procedure
is used to indicate the range of response of the Al(n,α)
8.1 Decide on the size and shape of aluminum sample to be
reaction. Refer to Guide E1018 for recommended sources for
irradiated. This is influenced by the irradiation space and the
the tabulated dosimetry cross sections.
expected production of Na. Calculate the expected produc-
5.6 Two competing activities, Al (2.25 (2) minute half-
tion rate of Na from the activation equation described in
life) and Mg (9.458 (12) minute half-life), are formed in the
Section 9, and adjust sample size and irradiation time so that
27 28 27 27
reactions Al(n,γ) Al and Al(n,p) Mg, respectively, but
the Na may be accurately counted. A trial irradiation is
these can be eliminated by waiting 2 h before counting.
recommended.
8.2 Determine a suitable irradiation time (see 8.1). Since
6. Apparatus
24 24
Na has a 14.958 h half-life, the Na activity will approach
6.1 NaI(T1) or High Resolution Gamma-Ray
equilibrium after a day of irradiation.
Spectrometer—Due to its high resolution, the germanium
8.3 Weigh the sample.
detector is useful when contaminant activities are present (see
Guide E181 and Test Method E1005).
8.4 Irradiate the sample for the predetermined time period.
6.2 Precision Balance, able to achieve the required accu- Record the power level and any changes in power during the
irradiation, the time at the beginning and end of the irradiation,
racy.
and the relative position of the monitors in the irradiation
7. Materials
facility.
7.1 The purity of the aluminum is important. No impurities
8.5 After irradiation, the sample should be thoroughly
should be present that produce long-lived gamma-ray-emitting
rinsed in warm water. This will remove any Na surface
radionuclides having gamma-ray energies that interfere with
contamination produced during irradiation.
the Na determination. Discard aluminum that contains such
8.6 Check the sample for activity from cross-contamination
impurities or that contains quantities of Na sufficient to
by other irradiated materials. Clean, if necessary, and reweigh.
interfere, through thermal-neutron capture, with Na determi-
nation. The presence of these impurities s
...
This document is not an ASTM standard and is intended only to provide the user of an ASTM standard an indication of what changes have been made to the previous version. Because
it may not be technically possible to adequately depict all changes accurately, ASTM recommends that users consult prior editions as appropriate. In all cases only the current version
of the standard as published by ASTM is to be considered the official document.
Designation: E266 − 17 E266 − 23
Standard Test Method for
Measuring Fast-Neutron Reaction Rates by Radioactivation
of Aluminum
This standard is issued under the fixed designation E266; the number immediately following the designation indicates the year of
original adoption or, in the case of revision, the year of last revision. A number in parentheses indicates the year of last reapproval. A
superscript epsilon (´) indicates an editorial change since the last revision or reapproval.
1. Scope
27 24
1.1 This test method covers procedures measuring reaction rates by the activation reaction Al(n,α) Na.
1.2 This activation reaction is useful for measuring neutrons with energies above approximately 6.5 MeV and for irradiation times
up to about 2two days (for longer irradiations, or when there are significant variations in reactor power during the irradiation, see
Practice E261).
6 −2 −1
1.3 With suitable techniques, fission-neutron fluence rates above 10 cm ·s can be determined.
1.4 Detailed procedures for other fast neutron detectors are referenced in Practice E261.
1.5 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.
1.6 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.
2. Referenced Documents
2.1 ASTM Standards:
E170 Terminology Relating to Radiation Measurements and Dosimetry
E177 Practice for Use of the Terms Precision and Bias in ASTM Test Methods
E181 Guide for Detector Calibration and Analysis of Radionuclides in Radiation Metrology for Reactor Dosimetry
E261 Practice for Determining Neutron Fluence, Fluence Rate, and Spectra by Radioactivation Techniques
E456 Terminology Relating to Quality and Statistics
E844 Guide for Sensor Set Design and Irradiation for Reactor Surveillance
E944 Guide for Application of Neutron Spectrum Adjustment Methods in Reactor Surveillance
E1005 Test Method for Application and Analysis of Radiometric Monitors for Reactor Vessel Surveillance
E1018 Guide for Application of ASTM Evaluated Cross Section Data File
This test method is under the jurisdiction of ASTM Committee E10 on Nuclear Technology and Applications and is the direct responsibility of Subcommittee E10.05
on Nuclear Radiation Metrology.
Current edition approved Aug. 1, 2017June 1, 2023. Published October 2017June 2023. Originally approved in 1965. Last previous edition approved in 20112017 as
E266 – 11.E266 – 17. DOI: 10.1520/E0266-17.10.1520/E0266-23.
For referenced ASTM standards, visit the ASTM website, www.astm.org, or contact ASTM Customer Service at service@astm.org. For Annual Book of ASTM Standards
volume information, refer to the standard’s Document Summary page on the ASTM website.
Copyright © ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States
E266 − 23
3. Terminology
3.1 Definitions:
3.1.1 Refer to Terminologies E170 and E456.
4. Summary of Test Method
24 27 24
4.1 High-purity aluminum is irradiated in a neutron field, thereby producing radioactive Na from the Al(n,α) Na activation
reaction.
4.2 The gamma rays emitted by the radioactive decay of Na are counted (see Test Methods Guide E181) and the reaction rate,
as defined by Practice E261, is calculated from the decay rate and irradiation conditions.
4.3 The neutron fluence rate above about 6.5 MeV can then be calculated from the spectral-weighted neutron activation cross
section as defined by Practice E261.
5. Significance and Use
5.1 Refer to Guide E844 for the selection, irradiation, and quality control of neutron dosimeters.
5.2 Refer to Practice E261 for a general discussion of the determination of fast-neutron fluence rate with threshold detectors.
27 3
5.3 Pure aluminum in the form of foil or wire is readily available and easily handled. Al has an abundance of 100 % (1)). .
24 4
5.4 Na has a half-life of 14.958 (2) h (2) and emits gamma rays with energies of 1.368630 (5) and 2.754049 (5)(13) MeV (2).
5.5 Fig. 1 shows a plot of the RussianInternational Reactor Dosimetry File (RRDF)and Fusion File (IRDFF-II) cross section (3,
27 24
4) versus neutron energy for the fast-neutron reaction Al(n,α) Na (3) along with a comparison to the current experimental
database (5, 6). This RRDF-2008 cross section is identical to what is found in the latest International Atomic Energy Agency
(IAEA) International Reactor Dosimetry and Fusion File, IRDFF-1.05 (7).While the RRDF-2008 and IRDFF-1.05 cross sections
extend from threshold up to 60 MeV, due to considerations of the available validation data, the energy region over which this
standard recommends use of this cross section for reactor dosimetry applications only extends from threshold at ~4.25 MeV up
to 20 MeV. This figure is for illustrative purposes and is used to indicate the range of response of the Al(n,α) reaction. Refer to
Guide E1018 for recommended sources for the tabulated dosimetry cross sections.
28 27
5.6 Two competing activities, Al (2.25 (2) minute half-life) and Mg, Mg (9.458 (12) minute half-life), are formed in the
27 28 27 27
reactions Al(n,γ) Al and Al(n,p) Mg, respectively, but these can be eliminated by waiting 2 h before counting.
27 24
FIG. 1 Al(n,α) Na Cross Section, from RRDF-2008/IRDFF-1.05IRDFF-II Library, with EXFOR Experimental Data
The boldface numbers in parentheses refer to a list of References at the end of this standard.
The value of uncertainty, in parenthesis, refers to the corresponding last digits, thus 14.958 (2) corresponds to 14.958 6 0.002.
E266 − 23
6. Apparatus
6.1 NaI(T1) or High Resolution Gamma-Ray Spectrometer. Spectrometer—Because ofDue to its high resolution, the germanium
detector is useful when contaminant activities are present (see Test Methods Guide E181 and Test Method E1005).
6.2 Precision Balance, able to achieve the required accuracy.
7. Materials
7.1 The purity of the aluminum is important. No impurities should be present that produce long-lived gamma-ray-emitting
radionuclides having gamma-ray energies that interfere with the Na determination. Discard aluminum that contains such
23 24
impurities or that contains quantities of Na sufficient to interfere, through thermal-neutron capture, with Na determination. The
presence of these impurities should be determined by activation analysis since spectrographically pure aluminum may contain a
contaminant not detectable by the emission spectrograph. If the Na content of the irradiated samples is determined from the
emission rate of the 2.754049 MeV gamma ray, the probability of interference from contaminant gamma rays is much less than
if the 1.368630 MeV gamma ray is used.
7.2 Encapsulating Materials—Brass, stainless steel, copper, aluminum, quartz, or vanadium have been used as primary
encapsulating materials. The container should be constructed in such a manner that it will not create significant flux perturbation
and that it may be opened easily, especially if the capsule is to be opened remotely (see Guide E844).
8. Procedure
8.1 Decide on the size and shape of aluminum sample to be irradiated. This is influenced by the irradiation space and the expected
24 24
production of Na. Calculate the expected production rate of Na from the activation equation described in Section 9, and adjust
sample size and irradiation time so that the Na may be accurately counted. A trial irradiation is recommended.
24 24
8.2 Determine a suitable irradiation time (see 8.1). Since Na has a 14.958 h half-life, the Na activity will approach equilibrium
after a day of irradiation.
8.3 Weigh the sample.
8.4 Irradiate the sample for the predetermined time period. Record the power level and any changes in power during the
irradiation, the time at the beginning and end of the irradiation, and the relative position of the monitors in the irradiation facility.
8.5 After irradiation, the sample should be thoroughly rinsed in warm water. This will remove any Na surface contamination
produced during irradiation.
8.6 Check the sample for activity from cross-contamination by other irradiated materials. Clean, if necessary, and reweigh.
24 28 27
8.7 Analyze the sampl
...








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