{"id":424331,"date":"2024-10-20T06:51:13","date_gmt":"2024-10-20T06:51:13","guid":{"rendered":"https:\/\/pdfstandards.shop\/product\/uncategorized\/bs-en-iec-608062022-tc-2023\/"},"modified":"2024-10-26T12:52:47","modified_gmt":"2024-10-26T12:52:47","slug":"bs-en-iec-608062022-tc-2023","status":"publish","type":"product","link":"https:\/\/pdfstandards.shop\/product\/publishers\/bsi\/bs-en-iec-608062022-tc-2023\/","title":{"rendered":"BS EN IEC 60806:2022 – TC 2023"},"content":{"rendered":"
This International Standard is applicable to X-RAY SOURCE ASSEMBLIES and X-RAY TUBE ASSEMBLIES, for use in MEDICAL DIAGNOSTIC RADIOLOGY for techniques in which the X-RAY PATTERN will be received simultaneously in all points of the IMAGE RECEPTION AREA. This standard specifies a method for the determination of the greatest geometrically symmetrical RADIATION FIELD at a specified distance from the FOCAL SPOT for which the percentage AIR KERMA RATE along the major axes of the RADIATION FIELD does not fall below a permitted value. NOTE 1 AIR KERMA or AIR KERMA RATE are the only practical verifiable physical quantities for X-RAY SOURCES. X-RAY SOURCES must be tested independently from MEDICAL ELECTRICAL SYSTEMS. Conversion to the characteristics of the X-RAY IMAGE RECEPTOR used in a MEDICAL ELECTRICAL SYSTEM may be done in addition. In case multiple FOCAL SPOTS are not super-imposed, each focal spot has its own REFERENCE AXIS. Then the maximum RADIATION FIELD may be given for each FOCAL SPOT separately NOTE 2 The maximum symmetrical RADIATION FIELD may change from its initial value as the X-RAY TUBE ages through use. NOTE 3 If, for certain MEDICAL ELECTRICAL SYSTEMs the scope of IEC 60806 does not fit, then the special RADIATION FIELD requirements could be incorporated in the MEDICAL ELECTRICAL SYSTEM particular standard. However, a statement on the RADIATION FIELD while referring IEC 60806 is then no longer possible.<\/p>\n
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1<\/td>\n | 30468447 <\/td>\n<\/tr>\n | ||||||
29<\/td>\n | A-30425847 <\/td>\n<\/tr>\n | ||||||
30<\/td>\n | undefined <\/td>\n<\/tr>\n | ||||||
35<\/td>\n | Annex ZA (normative)Normative references to international publicationswith their corresponding European publications <\/td>\n<\/tr>\n | ||||||
37<\/td>\n | English CONTENTS <\/td>\n<\/tr>\n | ||||||
38<\/td>\n | FOREWORD <\/td>\n<\/tr>\n | ||||||
40<\/td>\n | 1 Scope 2 Normative references <\/td>\n<\/tr>\n | ||||||
41<\/td>\n | 3 Terms and definitions 4 Maximum symmetrical radiation field 4.1 Orientation of the maximum symmetrical radiation field Figures Figure 1 \u2013 Orientation of the maximum symmetrical radiation field <\/td>\n<\/tr>\n | ||||||
42<\/td>\n | 4.2 Determination of the maximum symmetrical radiation field 5 Measurement of the distribution of air kerma rate 5.1 Detector Figure 2 \u2013 Typical distribution of the relative air kerma rate alongthe major axis X of a maximum symmetrical radiation field <\/td>\n<\/tr>\n | ||||||
43<\/td>\n | 5.2 Measuring arrangement Figure 3 \u2013 Measuring arrangement <\/td>\n<\/tr>\n | ||||||
44<\/td>\n | 5.3 Measuring conditions 6 Statement of compliance Table 1 \u2013 Radiation quality <\/td>\n<\/tr>\n | ||||||
45<\/td>\n | Annex A (informative)Background A.1 Overview A.2 Second edition <\/td>\n<\/tr>\n | ||||||
46<\/td>\n | Index of defined terms <\/td>\n<\/tr>\n<\/table>\n","protected":false},"excerpt":{"rendered":" Tracked Changes. Determination of the maximum symmetrical radiation field of X-ray tube assemblies and X-ray source assemblies for medical diagnosis<\/b><\/p>\n |