BS EN 60789-2005 Medical electrical equipment — Characteristics and test conditions of radionuclide imaging devices — Anger type gamma cameras《医用电气设备 放射性核素成像装置的性能和试验条件 ANGER型γ照相机》.pdf

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1、BRITISH STANDARDBS EN 60789:2005Medical electrical equipment Characteristics and test conditions of radionuclide imaging devices Anger type gamma camerasThe European Standard EN 60789:2005 has the status of a British StandardICS 11.040.50g49g50g3g38g50g51g60g44g49g42g3g58g44g55g43g50g56g55g3g37g54g4

2、4g3g51g40g53g48g44g54g54g44g50g49g3g40g59g38g40g51g55g3g36g54g3g51g40g53g48g44g55g55g40g39g3g37g60g3g38g50g51g60g53g44g42g43g55g3g47g36g58Licensed Copy: Wang Bin, na, Tue May 09 08:37:42 BST 2006, Uncontrolled Copy, (c) BSIBS EN 60789:2005This British Standard was published under the authority of th

3、e Standards Policy and Strategy Committee on 13 February 2006 BSI 13 February 2006ISBN 0 580 47176 4National forewordThis British Standard is the official English language version of EN 60789:2005. It is identical with IEC 60789:2005. It supersedes BS EN 60789:1994 which is withdrawn.The UK particip

4、ation in its preparation was entrusted by Technical Committee CH/62, Electromedical equipment in medical practice, to Subcommittee CH/62/3, Equipment for radiotherapy, nuclear medicine and radiation dosimetry, which has the responsibility to: A list of organizations represented on this subcommittee

5、can be obtained on request to its secretary.Cross-referencesThe British Standards which implement international or European publications referred to in this document may be found in the BSI Catalogue under the section entitled “International Standards Correspondence Index”, or by using the “Search”

6、facility of the BSI Electronic Catalogue or of British Standards Online.This publication does not purport to include all the necessary provisions of a contract. Users are responsible for its correct application. Compliance with a British Standard does not of itself confer immunity from legal obligat

7、ions. aid enquirers to understand the text; present to the responsible international/European committee any enquiries on the interpretation, or proposals for change, and keep UK interests informed; monitor related international and European developments and promulgate them in the UK.Summary of pages

8、This document comprises a front cover, an inside front cover, the EN title page, pages 2 to 29 and a back cover.The BSI copyright notice displayed in this document indicates when the document was last issued.Amendments issued since publicationAmd. No. Date CommentsLicensed Copy: Wang Bin, na, Tue Ma

9、y 09 08:37:42 BST 2006, Uncontrolled Copy, (c) BSIEUROPEAN STANDARD EN 60789 NORME EUROPENNE EUROPISCHE NORM December 2005 CENELEC European Committee for Electrotechnical Standardization Comit Europen de Normalisation Electrotechnique Europisches Komitee fr Elektrotechnische Normung Central Secretar

10、iat: rue de Stassart 35, B - 1050 Brussels 2005 CENELEC - All rights of exploitation in any form and by any means reserved worldwide for CENELEC members. Ref. No. EN 60789:2005 E ICS 11.040.50 Supersedes EN 60789:1993English version Medical electrical equipment Characteristics and test conditions of

11、 radionuclide imaging devices - Anger type gamma cameras (IEC 60789:2005) Appareils lectromdicaux - Caractristiques et conditions dessai des dispositifs dimagerie par radionuclides Gamma camras de type Anger (CEI 60789:2005) Medizinische elektrische Gerte - Merkmale und Prfbedingungen fr bildgebende

12、 Systeme in der Nuklearmedizin Einkristall-Gamma-Kameras (IEC 60789:2005) This European Standard was approved by CENELEC on 2005-11-01. CENELEC members are bound to comply with the CEN/CENELEC Internal Regulations which stipulate the conditions for giving this European Standard the status of a natio

13、nal standard without any alteration. Up-to-date lists and bibliographical references concerning such national standards may be obtained on application to the Central Secretariat or to any CENELEC member. This European Standard exists in three official versions (English, French, German). A version in

14、 any other language made by translation under the responsibility of a CENELEC member into its own language and notified to the Central Secretariat has the same status as the official versions. CENELEC members are the national electrotechnical committees of Austria, Belgium, Cyprus, Czech Republic, D

15、enmark, Estonia, Finland, France, Germany, Greece, Hungary, Iceland, Ireland, Italy, Latvia, Lithuania, Luxembourg, Malta, Netherlands, Norway, Poland, Portugal, Slovakia, Slovenia, Spain, Sweden, Switzerland and United Kingdom. Licensed Copy: Wang Bin, na, Tue May 09 08:37:42 BST 2006, Uncontrolled

16、 Copy, (c) BSIEN 60789:2005 2 Foreword The text of document 62C/388/FDIS, future edition 3 of IEC 60789, prepared by SC 62C, Equipment for radiotherapy, nuclear medicine and radiation dosimetry, of IEC TC 62, Electrical equipment in medical practice, was submitted to the IEC-CENELEC parallel vote an

17、d was approved by CENELEC as EN 60789 on 2005-11-01. This European Standard supersedes EN 60789:1993. With respect to EN 60789:1993, the measurement of intrinsic point source sensitivity variation has been removed, the subclauses SYSTEM SENSITIVITY (4.2), SPATIAL RESOLUTION (4.3), NON-UNIFORMITY OF

18、RESPONSE (4.5), INTRINSIC MULTIPLE WINDOW SPATIAL REGISTRATION (4.7) and COUNT RATE CHARACTERISTIC (4.8) have been reformulated (although the procedures are mostly unchanged) and some small editorial changes have been made. The following dates were fixed: latest date by which the EN has to be implem

19、ented at national level by publication of an identical national standard or by endorsement (dop) 2006-08-01 latest date by which the national standards conflicting with the EN have to be withdrawn (dow) 2008-11-01 In this standard the following print types are used: requirements, compliance with whi

20、ch can be tested, and definitions: in roman type; notes, explanations, advice, introductions, general statements, exceptions and reference: in smaller roman type; test specifications: in italic type; TERMS DEFINED IN CLAUSE 3 OF THIS STANDARD LISTED IN ANNEX B: SMALL CAPITALS. The requirements are f

21、ollowed by specifications for the relevant tests. Annex ZA has been added by CENELEC. _ Endorsement notice The text of the International Standard IEC 60789:2005 was approved by CENELEC as a European Standard without any modification. _ Licensed Copy: Wang Bin, na, Tue May 09 08:37:42 BST 2006, Uncon

22、trolled Copy, (c) BSI 3 EN 60789:2005 CONTENTS INTRODUCTION.4 1 Scope 5 2 Normative references .5 3 Terms and definitions .5 4 Test methods .8 4.1 General requirements 8 4.2 SYSTEM SENSITIVITY 8 4.3 SPATIAL RESOLUTION .10 4.4 SPATIAL NON-LINEARITY .12 4.5 NON-UNIFORMITY OF RESPONSE 13 4.6 INTRINSIC

23、ENERGY RESOLUTION.15 4.7 INTRINSIC MULTIPLE WINDOW SPATIAL REGISTRATION .15 4.8 COUNT RATE CHARACTERISTIC 17 4.9 Shield leakage test 18 5 ACCOMPANYING DOCUMENTS .19 Annex ZA (normative) Normative references to international publications with their Bibliography .26 Index of defined terms 27 Figure 1

24、Cuvette 19 Figure 2 Cylindrical phantom20 Figure 3 Uniform source.20 Figure 4 Slit phantom for measurement of intrinsic resolution and SPATIAL NON-LINEARITY 21 Figure 5 Source arrangement for intrinsic measurements (4.3.5, 4.4.1, 4.5.4 and 4.6) .22 Figure 6 Small shielded liquid source .23 Figure 7

25、Measurement of FWHM 24 Figure 8 Evaluation of EQUIVALENT WIDTH (EW)25 Table 1 Radionuclides and energy windows to be used for performance measurements8 corresponding European publications29 Licensed Copy: Wang Bin, na, Tue May 09 08:37:42 BST 2006, Uncontrolled Copy, (c) BSIEN 60789:2005 4 INTRODUCT

26、ION The test methods specified in this standard have been selected to reflect as much as possible the clinical use of GAMMA CAMERAS. It is intended that the test methods be carried out by manufacturers, thereby enabling them to describe the characteristics of GAMMA CAMERAS on a common basis. License

27、d Copy: Wang Bin, na, Tue May 09 08:37:42 BST 2006, Uncontrolled Copy, (c) BSI 5 EN 60789:2005 MEDICAL ELECTRICAL EQUIPMENT CHARACTERISTICS AND TEST CONDITIONS OF RADIONUCLIDE IMAGING DEVICES ANGER TYPE GAMMA CAMERAS 1 Scope This International Standard specifies test methods for declaring the charac

28、teristics of Anger type GAMMA CAMERAS. The latter are composed of a collimator, a detector shield and a radiation detector assembly, together with recording and display devices. It is not within the scope of this standard to address the safety requirements to be followed by manufacturers according t

29、o IEC 60601-1. 2 Normative references The following referenced documents are for the application of this document. For dated references, only the edition cited applies. For undated references, the latest edition of the referenced document (including any amendments) applies. IEC 60788:2004, Medical e

30、lectrical equipment Glossary of defined terms 3 Terms and definitions For the purposes of this document, the definitions given in IEC 60788 (see Index of defined terms) and the following apply. 3.1 ENERGY WINDOW range defining the energy signals accepted by the device for further processing 3.2 DETE

31、CTOR FIELD OF VIEW FOV region of the detector within which events are included in the display image, and for which all performance specifications are provided 3.3 COLLIMATOR FRONT FACE surface of the COLLIMATOR which is closest to the object being imaged 3.4 COLLIMATOR BACK FACE surface of the COLLI

32、MATOR which is closest to the RADIATION DETECTOR ASSEMBLY 3.5 ENTRANCE FIELD OF A COLLIMATOR area bounded by the shortest line which is tangential to the outside edges of the peripheral COLLIMATOR apertures on the COLLIMATOR FRONT FACE Licensed Copy: Wang Bin, na, Tue May 09 08:37:42 BST 2006, Uncon

33、trolled Copy, (c) BSIEN 60789:2005 6 3.6 EXIT FIELD OF A COLLIMATOR area bounded by the shortest line which is tangential to the outside edges of the peripheral COLLIMATOR apertures on the COLLIMATOR BACK FACE 3.7 COLLIMATOR AXIS straight line which passes through the geometrical centre of the EXIT

34、and ENTRANCE FIELDS of the COLLIMATOR 3.8 PARALLEL HOLE COLLIMATOR COLLIMATOR with a number of apertures, the axes of which are parallel 3.9 PIN-HOLE COLLIMATOR COLLIMATOR with one small aperture in a plane in front of the RADIATION DETECTOR ASSEMBLY 3.10 ADDRESS PILE UP false address calculation of

35、 an artificial event which passes the ENERGY WINDOW, but is formed from two or more events by the PILE UP EFFECT 3.11 PILE UP EFFECT false measurement of the pulse amplitude, due to the absorption of two or more gamma rays, reaching the same radiation detector within the RESOLVING TIME IEC 61675-1,

36、definition 2.7.4.1 3.12 SYSTEM SENSITIVITY with a specified COLLIMATOR and ENERGY WINDOW, the ratio of the COUNT RATE of the DETECTOR HEAD to the ACTIVITY of a plane source of specific dimensions and containing a specified radionuclide placed perpendicular to and centred on the COLLIMATOR AXIS under

37、 specified conditions NOTE See also Figure 2. 3.13 INTRINSIC LINE SPREAD FUNCTION line spread function measured with a collimated line source in front of the DETECTOR HEAD without COLLIMATOR 3.14 DETECTOR HEAD LINE SPREAD FUNCTION line spread function measured with an uncollimated line source at a s

38、pecified distance Z from the COLLIMATOR FRONT FACE 3.15 EQUIVALENT WIDTH EW width of a rectangle having the same area as the LSF and a height equal to the maximum value of the LSF Licensed Copy: Wang Bin, na, Tue May 09 08:37:42 BST 2006, Uncontrolled Copy, (c) BSI 7 EN 60789:2005 3.16 SPATIAL RESOL

39、UTION ability to concentrate the count density distribution in the image of a POINT SOURCE to a point IEC 61675-1, definition 2.4 3.17 SYSTEM SPATIAL RESOLUTION SPATIAL RESOLUTION in a scattering medium for a specified COLLIMATOR, or a specified radionuclide, and at a specified distance from the COL

40、LIMATOR FRONT FACE 3.18 INTRINSIC SPATIAL RESOLUTION SPATIAL RESOLUTION in air for a specified radionuclide excluding the COLLIMATOR 3.19 INTRINSIC ENERGY SPECTRUM measured histogram of pulse heights for the DETECTOR HEAD without COLLIMATOR NOTE The pulse height should be expressed as corresponding

41、energy. 3.20 INTRINSIC ENERGY RESOLUTION FULL WIDTH AT HALF MAXIMUM of the full energy absorption peak in the INTRINSIC ENERGY SPECTRUM for a specified radionuclide 3.21 MULTIPLE WINDOW SPATIAL REGISTRATION measured position of a source as a function of the ENERGY WINDOW setting 3.22 INTRINSIC NON-U

42、NIFORMITY OF RESPONSE NON-UNIFORMITY OF RESPONSE of the DETECTOR HEAD without COLLIMATOR 3.23 SYSTEM NON-UNIFORMITY OF RESPONSE NON-UNIFORMITY OF RESPONSE of the DETECTOR HEAD with COLLIMATOR 3.24 SPATIAL NON-LINEARITY deviations of the image of a straight line source from a straight line 3.25 INTRI

43、NSIC SPATIAL NON-LINEARITY SPATIAL NON-LINEARITY of the DETECTOR HEAD without COLLIMATOR 3.26 COUNT LOSS difference between measured COUNT RATE and TRUE COUNT RATE, which is caused by the finite RESOLVING TIME of the instrument IEC 61675-1, definition 2.7.1 Licensed Copy: Wang Bin, na, Tue May 09 08

44、:37:42 BST 2006, Uncontrolled Copy, (c) BSIEN 60789:2005 8 3.27 COUNT RATE number of counts per unit of time IEC 61675-1, definition 2.7.2 4 Test methods 4.1 General requirements All measurements shall be performed with the energy window settings specified in Table 1. Table 1 Radionuclides and energ

45、y windows to be used for performance measurements Radionuclide Energy window keV 99mTc 141, with a tolerance of 7,5 % 131I 364, with a tolerance of 10 % 67Ga 93, 184, 300, with a tolerance of 20 % 68Ga 511, with a tolerance of 10 % NOTE Because the characteristics of a gamma camera may change notice

46、ably between 122 keV (57Co) and 141 keV (99mTc), the former is not included as a suitable radionuclide. However, it may be useful in some circumstances, e.g. for quality control. Additional measurements with other settings, as specified by the manufacturer, can be performed. Before the measurements

47、are performed, the camera shall be adjusted by the procedure normally used by the manufacturer for an installed unit and shall not be adjusted specially for the measurement of specific parameters. Unless otherwise specified, measurements shall be carried out at count rates not exceeding 20 000 count

48、s per second. 4.2 SYSTEM SENSITIVITY 4.2.1 General Sensitivity is a parameter that characterizes the effectiveness of a system to identify the radiation emitted from a RADIOACTIVE SOURCE, i.e. the rate at which events are detected in the presence of a RADIOACTIVE SOURCE in the limit of low ACTIVITY

49、where COUNT LOSSES are negligible. The measured COUNT RATE for a given ACTIVITY and RADIONUCLIDE depends on many factors, including the detector material, its size and thickness, the size and shape of the RADIOACTIVE SOURCE including its absorption and scatter properties, and instruments dead time, energy thresholds and COLLIMATOR. 4.2.2 Purpose The purpose of this measurement is to determine the detected rate of events per unit of ACTIVITY for a standard volume sour

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