ISO/FDIS 24459
(Main)Determination of uranium content in samples coming from the nuclear fuel cycle by L-absorption edge spectrometry
Determination of uranium content in samples coming from the nuclear fuel cycle by L-absorption edge spectrometry
Détermination de l'uranium dans les solutions du cycle du combustible nucléaire par absorption de rayons X à la discontinuité L
General Information
Standards Content (sample)
FINAL
INTERNATIONAL ISO/FDIS
DRAFT
STANDARD 24459
ISO/TC 85/SC 5
Determination of uranium content in
Secretariat: BSI
samples coming from the nuclear fuel
Voting begins on:
20210706 cycle by L-absorption edge
spectrometry
Voting terminates on:
20210831
Détermination de l'uranium dans les solutions du cycle du
combustible nucléaire par absorption de rayons X à la discontinuité L
RECIPIENTS OF THIS DRAFT ARE INVITED TO
SUBMIT, WITH THEIR COMMENTS, NOTIFICATION
OF ANY RELEVANT PATENT RIGHTS OF WHICH
THEY ARE AWARE AND TO PROVIDE SUPPOR TING
DOCUMENTATION.
IN ADDITION TO THEIR EVALUATION AS
Reference number
BEING ACCEPTABLE FOR INDUSTRIAL, TECHNO
ISO/FDIS 24459:2021(E)
LOGICAL, COMMERCIAL AND USER PURPOSES,
DRAFT INTERNATIONAL STANDARDS MAY ON
OCCASION HAVE TO BE CONSIDERED IN THE
LIGHT OF THEIR POTENTIAL TO BECOME STAN
DARDS TO WHICH REFERENCE MAY BE MADE IN
NATIONAL REGULATIONS. ISO 2021
---------------------- Page: 1 ----------------------
ISO/FDIS 24459:2021(E)
COPYRIGHT PROTECTED DOCUMENT
© ISO 2021
All rights reserved. Unless otherwise specified, or required in the context of its implementation, no part of this publication may
be reproduced or utilized otherwise in any form or by any means, electronic or mechanical, including photocopying, or posting
on the internet or an intranet, without prior written permission. Permission can be requested from either ISO at the address
below or ISO’s member body in the country of the requester.ISO copyright office
CP 401 • Ch. de Blandonnet 8
CH1214 Vernier, Geneva
Phone: +41 22 749 01 11
Email: copyright@iso.org
Website: www.iso.org
Published in Switzerland
ii © ISO 2021 – All rights reserved
---------------------- Page: 2 ----------------------
ISO/FDIS 24459:2021(E)
Contents Page
Foreword ........................................................................................................................................................................................................................................iv
1 Scope ................................................................................................................................................................................................................................. 1
2 Normative references ...................................................................................................................................................................................... 1
3 Terms and definitions ..................................................................................................................................................................................... 1
4 Principle ........................................................................................................................................................................................................................ 1
5 Reagents and materials ................................................................................................................................................................................. 2
6 Apparatus ..................................................................................................................................................................................................................... 2
7 Method ............................................................................................................................................................................................................................ 4
7.1 Prechecks ................................................................................................................................................................................................... 4
7.2 Reference spectrum ............................................................................................................................................................................ 4
7.3 Calibration .................................................................................................................................................................................................. 4
7.4 Sample measurement ........................................................................................................................................................................ 5
7.5 Spectrum evaluation .......................................................................................................................................................................... 5
7.5.1 Region of interest ............................................................................................................................................................ 5
7.5.2 Smoothing (optional) ................................................................................................................................................. 5
7.5.3 Background subtraction ............................................................................................................................................ 6
7.5.4 Calculation of the X-ray transmission ............................................................................................................ 6
7.6 Calculation of the concentration of uranium ................................................................................................................ 7
7.7 Quality control ......................................................................................................................................................................................... 8
7.8 Uncertainty evaluation ..................................................................................................................................................................... 8
7.8.1 Standard uncertainty of the calibration factor ...................................................................................... 8
7.8.2 Standard uncertainty of the uranium concentration ........................................................................ 9
Annex A (informative) Calculation method for correction factors of atomic mass and
temperature ...........................................................................................................................................................................................................10
Annex B (informative) Preparation of a solid quality control sample............................................................................11
Bibliography .............................................................................................................................................................................................................................13
© ISO 2021 – All rights reserved iii---------------------- Page: 3 ----------------------
ISO/FDIS 24459:2021(E)
Foreword
ISO (the International Organization for Standardization) is a worldwide federation of national standards
bodies (ISO member bodies). The work of preparing International Standards is normally carried out
through ISO technical committees. Each member body interested in a subject for which a technical
committee has been established has the right to be represented on that committee. International
organizations, governmental and nongovernmental, in liaison with ISO, also take part in the work.
ISO collaborates closely with the International Electrotechnical Commission (IEC) on all matters of
electrotechnical standardization.The procedures used to develop this document and those intended for its further maintenance are
described in the ISO/IEC Directives, Part 1. In particular, the different approval criteria needed for the
different types of ISO documents should be noted. This document was drafted in accordance with the
editorial rules of the ISO/IEC Directives, Part 2 (see www .iso .org/ directives).
Attention is drawn to the possibility that some of the elements of this document may be the subject of
patent rights. ISO shall not be held responsible for identifying any or all such patent rights. Details of
any patent rights identified during the development of the document will be in the Introduction and/or
on the ISO list of patent declarations received (see www .iso .org/ patents).Any trade name used in this document is information given for the convenience of users and does not
constitute an endorsement.For an explanation of the voluntary nature of standards, the meaning of ISO specific terms and
expressions related to conformity assessment, as well as information about ISO's adherence to the
World Trade Organization (WTO) principles in the Technical Barriers to Trade (TBT) see www .iso .org/
iso/ foreword .html.This document was prepared by Technical Committee ISO/TC 85, Nuclear energy, nuclear technologies,
and radio protection, Subcommittee SC 5, Analytical methodology in the nuclear fuel cycle.
Any feedback or questions on this document should be directed to the user’s national standards body. A
complete listing of these bodies can be found at www .iso .org/ members .html.iv © ISO 2021 – All rights reserved
---------------------- Page: 4 ----------------------
FINAL DRAFT INTERNATIONAL STANDARD ISO/FDIS 24459:2021(E)
Determination of uranium content in samples coming from
the nuclear fuel cycle by L-absorption edge spectrometry
1 Scope
This document specifies a method for the determination of uranium concentrations in nitric acid or
TBP-DILUANT (for example TBP-kerosene) solutions coming from the nuclear fuel cycle.
The method is applicable— for process control to solutions, free of suspension, which contain between 10 g/l to 300 g/l uranium,
and— for high accuracy purposes (Safeguards) to nitric acid solutions, free of suspension, which contain
between 100 g/l and 220 g/l uranium.Having
— the content of neptunium and plutonium impurities in the solution less than 1 % of the uranium
content.— the content of neutron poisons (gadolinium, erbium) less than 1 % of the uranium content to ensure
the absence of significant interferences at the level of required precision, for high accuracy purposes.
The method is applicable to solid samples as well, provided that they can be fully dissolved in nitric
acid.2 Normative references
There are no normative references in this document.
3 Terms and definitions
No terms and definitions are listed in this document.
ISO and IEC maintain terminological databases for use in standardization at the following addresses:
— ISO Online browsing platform: available at https:// www .iso .org/ obp— IEC Electropedia: available at https:// www .electropedia .org/
4 Principle
A highly collimated X-ray beam passes through a uranium solution with well-defined path length.
The transmission spectrum is recorded with a solid-state detector. A sharp jump of the photon
transmission, which is related to the concentration of uranium, occurs at the L-edge energy of uranium
(E = 17,17 keV). Uranium concentration is determined from the size of the jump using calibration and
LIIIspectrum processing algorithms.
The proposed spectrum processing algorithms require the acquisition of reference spectrum to cancel
out the influence of the matrix.For high accuracy measurement, the isotopic composition of uranium and the temperature shall be
known and corrections may apply.© ISO 2021 – All rights reserved 1
---------------------- Page: 5 ----------------------
ISO/FDIS 24459:2021(E)
The uncertainty of the number of counts in the channels before and after the L-edge is one of the main
contributors to the measurement uncertainty.The acquisition time needed to reach the necessary number of counts depends of the total count
rate. The total count rate is a function of the intensity of the X-ray generator, of the characteristic of
instrument, and of the concentration of uranium.It is therefore specific to the laboratory, which shall evaluate beforehand the fit-for-purpose accuracy
that will decide the target total count in the spectrum, the count rate and the acquisition time.
For high accuracy measurements, a minimum total number of counts of 2 000 000 in the fitting window
is required to ensure satisfactory statistics around the L-edge. The count rates and measurement times
given as indication in the document reflect this requirement. The reference, calibration and sample
spectra shall be recorded with the same count rate and the same high voltage (HV) cutoff.
For process control purposes, the necessary total number of counts will depend of the needed accuracy.
The measurement should be performed at the same HV cutoff and current.5 Reagents and materials
Only analytical grade reagents shall be used.
All aqueous solutions shall be prepared with distilled water or deionized water.
5.1 Nitric acid solutions, c(HNO )≈3 mol/l, prepared from w(HNO ) 65 %, ρ= 1,42 g/cm .
3 35.2 Uranium reference solutions.
These solutions are used for calibration and quality control purposes. They should ideally be prepared
from a solid or liquid material with known uranium concentration, and known uranium isotopic
composition for high accuracy purposes. The standard uncertainty of the uranium concentration
should be equal or better than 0,06 %. The use of certified reference material traceable to SI units is
recommended.6 Apparatus
The L-absorption edge spectrometer consists of an X-ray tube, an X-ray detector, a multichannel
analyser, a temperature sensor and software for data acquisition and processing. A principle diagram
of the instrument components is shown in Figure 1.2 © ISO 2021 – All rights reserved
---------------------- Page: 6 ----------------------
ISO/FDIS 24459:2021(E)
Key
1 HV controller 6 detector
2 X-ray tube 7 MCA
3 collimator 8 sample cell
4 temperature sensor 9 computer
5 collimator
Figure 1 — Schematic of the instrument components
6.1 X-ray tube.
The maximum working voltage of X-ray tube is higher than 25 kV, voltage-controlled, current-controlled.
It shall be stable over time and shall reach an intensity (adjustable, usually lower than 100 μA) high
enough to ensure satisfactory total count rate for fast and accurate measurement (as described in
Clause 4).6.2 Shielding and collimator.
The shielding body is made of brass or other shield materials. X-ray tube, X-ray detector and sample cell
are directly mounted in the shielding body. The thickness of the shielding is chosen to ensure no X-ray
leakage, and to satisfy the radioprotection requirements.The collimator is made of tungsten, or other materials, whose fluorescence X-rays do not interfere with
the region of interest.6.3 Sample cell.
The sample cell can be made of glass or polycarbonate (PC), which can withstand nitric acid and TBP-
DILUANT or in quartz that is resistant to nitric acid.The optimum path length and the specifications of the cell depend on the characteristic of the apparatus
and the analytical needs.Examples of cell specifications:
— for process control purposes, disposable 4mm long PC cell;
— for high accuracy purposes, fixed flow-through cell with a path len
...
Questions, Comments and Discussion
Ask us and Technical Secretary will try to provide an answer. You can facilitate discussion about the standard in here.