{"id":416371,"date":"2024-10-20T06:10:22","date_gmt":"2024-10-20T06:10:22","guid":{"rendered":"https:\/\/pdfstandards.shop\/product\/uncategorized\/bsi-pd-iec-pas-634462022\/"},"modified":"2024-10-26T11:28:04","modified_gmt":"2024-10-26T11:28:04","slug":"bsi-pd-iec-pas-634462022","status":"publish","type":"product","link":"https:\/\/pdfstandards.shop\/product\/publishers\/bsi\/bsi-pd-iec-pas-634462022\/","title":{"rendered":"BSI PD IEC PAS 63446:2022"},"content":{"rendered":"
PDF Pages<\/th>\n | PDF Title<\/th>\n<\/tr>\n | ||||||
---|---|---|---|---|---|---|---|
2<\/td>\n | undefined <\/td>\n<\/tr>\n | ||||||
4<\/td>\n | CONTENTS <\/td>\n<\/tr>\n | ||||||
5<\/td>\n | FOREWORD <\/td>\n<\/tr>\n | ||||||
7<\/td>\n | INTRODUCTION <\/td>\n<\/tr>\n | ||||||
8<\/td>\n | 1 Scope 2 Normative references <\/td>\n<\/tr>\n | ||||||
9<\/td>\n | 3 Terms and definitions <\/td>\n<\/tr>\n | ||||||
11<\/td>\n | 4 Symbols and abbreviated terms 4.1 Physical quantities <\/td>\n<\/tr>\n | ||||||
12<\/td>\n | 4.2 Constants 4.3 Abbreviations 5 Application of this document <\/td>\n<\/tr>\n | ||||||
13<\/td>\n | 6 APD conversion method by evaluation of the SAR distribution 7 Uncertainty estimation 7.1 Measurement uncertainty Tables Table 1 \u2013 Conversion factors for psSAR to psAPD <\/td>\n<\/tr>\n | ||||||
14<\/td>\n | 7.2 Numerical uncertainty 8 Measurement and computational report Table 2 \u2013 Uncertainty budget template for evaluating the uncertainty in the measured value of the psAPD of a DUT or validation antenna <\/td>\n<\/tr>\n | ||||||
15<\/td>\n | Annex A (informative)Rationale for conversion of psSAR into psAPD <\/td>\n<\/tr>\n | ||||||
16<\/td>\n | Annex B (informative)Poynting vector and absorbed power density B.1 Introduction B.2 Electric fields and magnetic fields in a lossy half space <\/td>\n<\/tr>\n | ||||||
17<\/td>\n | B.3 Power density absorbed in the lossy half space <\/td>\n<\/tr>\n | ||||||
18<\/td>\n | B.4 Power transmitted by the Poynting vector of the TE-waves <\/td>\n<\/tr>\n | ||||||
19<\/td>\n | B.5 Power transmitted by the Poynting vector of the TM-waves <\/td>\n<\/tr>\n | ||||||
20<\/td>\n | B.6 Summary <\/td>\n<\/tr>\n | ||||||
21<\/td>\n | Annex C (normative)Reference dipoles and psAPD values for system check and validation C.1 System check and validation C.2 Reference dipoles Figure C.1 \u2013 Mechanical details of the standard dipoles <\/td>\n<\/tr>\n | ||||||
22<\/td>\n | C.3 Numerical model of the system check dipoles Table C.1 \u2013 Mechanical dimensions of the reference dipoles Table C.2 \u2013 Parameters of the dielectric components ofthe CAD models of the reference dipoles Table C.3 \u2013Numerical psAPD target values (rotating square)and the values converted from numerical psSAR results <\/td>\n<\/tr>\n | ||||||
23<\/td>\n | Annex D (normative)Supplemental files and their checksums <\/td>\n<\/tr>\n | ||||||
24<\/td>\n | Bibliography <\/td>\n<\/tr>\n<\/table>\n","protected":false},"excerpt":{"rendered":" Conversion method of specific absorption rate to absorbed power density for the assessment of human exposure to radio frequency electromagnetic fields from wireless devices in close proximity to the head and body. Frequency range of 6 GHz to 10 GHz<\/b><\/p>\n |