IEC/IEEE 63195-2:2022
(Main)Assessment of power density of human exposure to radio frequency fields from wireless devices in close proximity to the head and body (frequency range of 6 GHz to 300 GHz) - Part 2: Computational procedure
Assessment of power density of human exposure to radio frequency fields from wireless devices in close proximity to the head and body (frequency range of 6 GHz to 300 GHz) - Part 2: Computational procedure
IEC/IEEE 63195-2:2022 specifies computational procedures for conservative and reproducible computations of power density (PD) incident to a human head or body due to radio-frequency (RF) electromagnetic field (EMF) transmitting devices. The computational procedures described are finite-difference time-domain (FDTD) and finite element methods (FEM), which are computational techniques that can be used to determine electromagnetic quantities by solving Maxwell’s equations within a specified computational uncertainty. The procedures specified here apply to exposure assessments for a significant majority of the population during the use of hand-held and body-worn RF transmitting devices. The methods apply to devices that can feature single or multiple transmitters or antennas, and that can be operated with their radiating part or parts at distances up to 200 mm from a human head or body.
This document can be employed to determine conformity with any applicable maximum PD requirements of different types of RF transmitting devices used in close proximity to the head and body, including those combined with other RF transmitting or non-transmitting devices or accessories (e.g. belt-clip), or embedded in garments. The overall applicable frequency range of these protocols and procedures is from 6 GHz to 300 GHz.
The RF transmitting device categories covered in this document include but are not limited to mobile telephones, radio transmitters in personal computers, desktop and laptop devices, and multi-band and multi-antenna devices.
The procedures of this document do not apply to PD assessment of electromagnetic fields emitted or altered by devices or objects intended to be implanted in the body.
NOTE For the assessment of the combined exposure from simultaneous transmitters at frequencies below 6 GHz, the relevant standards for SAR computation are IEC/IEEE 62704-1:2017 and IEC/IEEE 62704-4:2020.
This publication is published as an IEC/IEEE Dual Logo standard.
Evaluation de la densité de puissance de l'exposition humaine aux champs radiofréquences provenant de dispositifs sans fil à proximité immédiate de la tête et du corps (plage de fréquences de 6 ghz à 300 ghz) - Partie 2: Procédure de calcul
IEC/IEEE 63195-2:2022 spécifie les procédures de calcul pour des calculs conservateurs et reproductibles de la densité de puissance (PD, Power Density) incidente sur la tête ou le corps humain, provenant de dispositifs de transmission par champ électromagnétique (EMF, Electromagnetic Field) radiofréquence (RF). Les procédures de calcul décrites appliquent la méthode des différences finies dans le domaine temporel (FDTD, Finite-Difference Time‑Domain) ou la méthode des éléments finis (FEM, Finite Element Methods), qui sont des techniques de calcul pouvant être utilisées pour déterminer les grandeurs électromagnétiques en résolvant les équations de Maxwell dans une incertitude de calcul spécifiée. Les procédures spécifiées dans le présent document s'appliquent à l'évaluation de l'exposition d'une vaste majorité de la population lors de l'utilisation de dispositifs qui émettent des RF tenus à la main et portés sur le corps. Les méthodes s'appliquent aux dispositifs qui peuvent comporter un ou plusieurs émetteurs ou, et qui peuvent être utilisés alors que leurs parties rayonnantes se trouvent à des distances inférieures ou égales à 200 mm de la tête ou du corps humain.
Le présent document peut être utilisé pour déterminer la conformité aux exigences en matière de densité de puissance maximale applicables de différents types de dispositifs qui émettent des RF lorsqu'ils sont utilisés à proximité immédiate de la tête et du corps, y compris s'ils sont combinés à d'autres dispositifs ou accessoires qui émettent des RF ou non (clip de ceinture, par exemple) ou s'ils sont intégrés dans des vêtements. La plage de fréquences globale applicable pour ces protocoles et procédures est comprise entre 6 GHz et 300 GHz.
Les catégories de dispositifs qui émettent des RF couvertes par le présent document incluent notamment les téléphones mobiles, les émetteurs radio des ordinateurs personnels, les dispositifs de bureau et les dispositifs portables, ainsi que les dispositifs multibandes et multiantennes.
Les procédures du présent document ne s'appliquent pas à l'évaluation de la densité de puissance des champs électromagnétiques émis ou altérés par des dispositifs ou des objets destinés à être implantés dans le corps.
NOTE Pour l'évaluation de l'exposition combinée en provenance de plusieurs émetteurs simultanés qui fonctionnent à des fréquences inférieures à 6 GHz, les normes applicables pour les calculs du DAS sont l'IEC/IEEE 62704-1:2017 et l'IEC/IEEE 62704-4:2020.
Cette publication est publiée en tant que norme IEC/IEEE Dual Logo.
General Information
- Status
- Published
- Publication Date
- 10-May-2022
- Technical Committee
- TC 106 - Methods for the assessment of electric, magnetic and electromagnetic fields associated with human exposure
- Drafting Committee
- JWG 11 - TC 106/JWG 11
- Current Stage
- PPUB - Publication issued
- Start Date
- 11-May-2022
- Completion Date
- 27-May-2022
Overview
IEC/IEEE 63195-2:2022 is an international standard that specifies computational procedures for assessing power density (PD) of human exposure to radio frequency (RF) electromagnetic fields emitted by wireless devices operating in the frequency range of 6 GHz to 300 GHz. This standard focuses on close proximity scenarios where RF transmitting devices-such as mobile phones, laptops, and multi-antenna systems-are used near the human head or body, up to a distance of 200 mm.
The standard provides reproducible, conservative methods employing advanced computational techniques such as the finite-difference time-domain (FDTD) and finite element methods (FEM). These methods solve Maxwell’s equations within defined computational uncertainties to offer reliable exposure assessments for a majority of users. IEC/IEEE 63195-2:2022 is designed for conformity verification with maximum allowed PD limits, promoting safe use of wireless devices in everyday contexts.
Key Topics
- Computational Procedures: Detailed methodologies using FDTD and FEM for calculating power density incident on human tissue.
- Exposure Metrics and Parameters: Definitions and measurement units critical for accurate assessment of RF exposure near the head and body.
- Model Development and Validation: Guidance on creating device-under-test (DUT) numerical models, power normalization, and ensuring model validation with test equipment.
- Evaluation Surfaces and Averaging: Techniques for defining evaluation areas and methods to average power density for consistent exposure metrics.
- Uncertainty Evaluation: Comprehensive approach to quantifying uncertainties arising from computational parameters, model fidelity, mesh resolution, and dielectric properties.
- Multi-Antenna Devices: Procedures to handle RF exposure from devices with multiple transmitters or antennas, including simultaneous and non-simultaneous operation.
- Reporting Requirements: Standardized reporting format to ensure transparency and regulatory compliance.
Applications
IEC/IEEE 63195-2:2022 is essential for stakeholders involved in wireless device design, safety testing, certification, and regulatory compliance. Key applications include:
- Product Safety Testing: Enables manufacturers to accurately assess power density exposure from devices such as smartphones, tablets, laptops, and wearable technology.
- Regulatory Compliance: Provides standardized computational approaches for meeting international PD exposure limits set by health and safety authorities.
- Research and Development: Supports engineering teams developing new wireless technologies requiring advanced electromagnetic exposure analysis.
- Multi-Device Exposure Assessment: Facilitates evaluation of combined exposure effects from multiple transmitters or accessories worn close to the body.
- Wireless System Optimization: Helps in designing antenna configurations and device placements that minimize human exposure to RF fields.
Related Standards
- IEC/IEEE 62704-1:2017 & IEC/IEEE 62704-4:2020: These standards cover Specific Absorption Rate (SAR) assessment and computational procedures for frequencies below 6 GHz, complementing IEC/IEEE 63195-2:2022 which addresses higher frequencies (6 GHz to 300 GHz).
- IEC/IEEE 63195-1: Part 1 of the assessment series covering measurement methodologies for power density from wireless devices.
- Other IEC/IEEE RF Exposure Standards: These offer comprehensive frameworks for evaluating human exposure across different frequency bands and device types.
By adhering to IEC/IEEE 63195-2:2022, industry professionals ensure rigorous, uniform, and accurate computational evaluation of RF power density exposure, helping safeguard public health in an increasingly wireless world.
Keywords: IEC/IEEE 63195-2, power density assessment, radio frequency fields, RF exposure, wireless devices, computational procedure, FDTD, finite element method, electromagnetic field, human exposure, 6 GHz to 300 GHz, device testing, PD compliance, multi-antenna devices, RF safety standards.
IEC/IEEE 63195-2:2022 - Assessment of power density of human exposure to radio frequency fields from wireless devices in close proximity to the head and body (frequency range of 6 GHz to 300 GHz) - Part 2: Computational procedure
Frequently Asked Questions
IEC/IEEE 63195-2:2022 is a standard published by the International Electrotechnical Commission (IEC). Its full title is "Assessment of power density of human exposure to radio frequency fields from wireless devices in close proximity to the head and body (frequency range of 6 GHz to 300 GHz) - Part 2: Computational procedure". This standard covers: IEC/IEEE 63195-2:2022 specifies computational procedures for conservative and reproducible computations of power density (PD) incident to a human head or body due to radio-frequency (RF) electromagnetic field (EMF) transmitting devices. The computational procedures described are finite-difference time-domain (FDTD) and finite element methods (FEM), which are computational techniques that can be used to determine electromagnetic quantities by solving Maxwell’s equations within a specified computational uncertainty. The procedures specified here apply to exposure assessments for a significant majority of the population during the use of hand-held and body-worn RF transmitting devices. The methods apply to devices that can feature single or multiple transmitters or antennas, and that can be operated with their radiating part or parts at distances up to 200 mm from a human head or body. This document can be employed to determine conformity with any applicable maximum PD requirements of different types of RF transmitting devices used in close proximity to the head and body, including those combined with other RF transmitting or non-transmitting devices or accessories (e.g. belt-clip), or embedded in garments. The overall applicable frequency range of these protocols and procedures is from 6 GHz to 300 GHz. The RF transmitting device categories covered in this document include but are not limited to mobile telephones, radio transmitters in personal computers, desktop and laptop devices, and multi-band and multi-antenna devices. The procedures of this document do not apply to PD assessment of electromagnetic fields emitted or altered by devices or objects intended to be implanted in the body. NOTE For the assessment of the combined exposure from simultaneous transmitters at frequencies below 6 GHz, the relevant standards for SAR computation are IEC/IEEE 62704-1:2017 and IEC/IEEE 62704-4:2020. This publication is published as an IEC/IEEE Dual Logo standard.
IEC/IEEE 63195-2:2022 specifies computational procedures for conservative and reproducible computations of power density (PD) incident to a human head or body due to radio-frequency (RF) electromagnetic field (EMF) transmitting devices. The computational procedures described are finite-difference time-domain (FDTD) and finite element methods (FEM), which are computational techniques that can be used to determine electromagnetic quantities by solving Maxwell’s equations within a specified computational uncertainty. The procedures specified here apply to exposure assessments for a significant majority of the population during the use of hand-held and body-worn RF transmitting devices. The methods apply to devices that can feature single or multiple transmitters or antennas, and that can be operated with their radiating part or parts at distances up to 200 mm from a human head or body. This document can be employed to determine conformity with any applicable maximum PD requirements of different types of RF transmitting devices used in close proximity to the head and body, including those combined with other RF transmitting or non-transmitting devices or accessories (e.g. belt-clip), or embedded in garments. The overall applicable frequency range of these protocols and procedures is from 6 GHz to 300 GHz. The RF transmitting device categories covered in this document include but are not limited to mobile telephones, radio transmitters in personal computers, desktop and laptop devices, and multi-band and multi-antenna devices. The procedures of this document do not apply to PD assessment of electromagnetic fields emitted or altered by devices or objects intended to be implanted in the body. NOTE For the assessment of the combined exposure from simultaneous transmitters at frequencies below 6 GHz, the relevant standards for SAR computation are IEC/IEEE 62704-1:2017 and IEC/IEEE 62704-4:2020. This publication is published as an IEC/IEEE Dual Logo standard.
IEC/IEEE 63195-2:2022 is classified under the following ICS (International Classification for Standards) categories: 17.220.20 - Measurement of electrical and magnetic quantities. The ICS classification helps identify the subject area and facilitates finding related standards.
You can purchase IEC/IEEE 63195-2:2022 directly from iTeh Standards. The document is available in PDF format and is delivered instantly after payment. Add the standard to your cart and complete the secure checkout process. iTeh Standards is an authorized distributor of IEC standards.
Standards Content (Sample)
IEC/IEEE 63195-2 ®
Edition 1.0 2022-05
INTERNATIONAL
STANDARD
NORME
INTERNATIONALE
colour
inside
Assessment of power density of human exposure to radio frequency fields from
wireless devices in close proximity to the head and body (frequency range of
6 GHz to 300 GHz) –
Part 2: Computational procedure
Évaluation de la densité de puissance de l'exposition humaine aux champs
radiofréquences provenant de dispositifs sans fil à proximité immédiate de la
tête et du corps (plage de fréquences de 6 GHz à 300 GHz) –
Partie 2: Procédure de calcul
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IEC/IEEE 63195-2 ®
Edition 1.0 2022-05
INTERNATIONAL
STANDARD
NORME
INTERNATIONALE
colour
inside
Assessment of power density of human exposure to radio frequency fields from
wireless devices in close proximity to the head and body (frequency range of
6 GHz to 300 GHz) –
Part 2: Computational procedure
Évaluation de la densité de puissance de l'exposition humaine aux champs
radiofréquences provenant de dispositifs sans fil à proximité immédiate de la
tête et du corps (plage de fréquences de 6 GHz à 300 GHz) –
Partie 2: Procédure de calcul
INTERNATIONAL
ELECTROTECHNICAL
COMMISSION
COMMISSION
ELECTROTECHNIQUE
INTERNATIONALE
ICS 17.220.20 ISBN 978-2-8322-0184-8
– 2 – IEC/IEEE 63195-2:2022 © IEC/IEEE 2022
CONTENTS
FOREWORD . 6
INTRODUCTION . 8
1 Scope . 9
2 Normative references . 9
3 Terms and definitions . 10
3.1 Exposure metrics and parameters . 10
3.2 Spatial, physical, and geometrical parameters associated with exposure
metrics . 11
3.3 Test device technical operating and antenna parameters . 13
3.4 Computational parameters . 13
3.5 Uncertainty parameters . 14
4 Symbols and abbreviated terms . 14
4.1 Symbols . 14
4.1.1 Physical quantities . 14
4.1.2 Constants . 15
4.2 Abbreviated terms . 15
5 Overview and application of this document . 16
5.1 Overview of the numerical evaluation . 16
5.2 Application of this document . 17
5.3 Stipulations . 18
6 Requirements on the numerical software . 18
7 Model development and validation . 19
7.1 General . 19
7.2 Development of the numerical model of the DUT. 19
7.3 Power normalization . 20
7.4 Requirements on the experimental test equipment for model validation . 22
7.4.1 General . 22
7.4.2 Ambient conditions and device holder . 23
7.4.3 Power measurement . 23
7.5 Testing configurations for the validation of the DUT model . 24
7.5.1 General . 24
7.5.2 Tests to be performed . 24
7.5.3 Determining the validity of the DUT model . 25
7.5.4 Test reduction for additional DUTs . 25
8 Power density computation and averaging . 26
8.1 Evaluation surface . 26
8.2 Tests to be performed and DUT configurations . 26
8.2.1 General . 26
8.2.2 Devices with a single radiating element or with multiple elements that
do not operate simultaneously . 27
8.2.3 Devices with antenna arrays or sub-arrays . 27
8.2.4 Devices with multiple antennas or multiple transmitters . 28
8.3 Considerations on the evaluation surface and dimensions of the
computational domain . 29
8.4 Averaging of power density on an evaluation surface . 29
8.4.1 General . 29
8.4.2 Construction of the averaging area on an evaluation surface . 30
8.5 Computation of sPD by integration of the Poynting vector. 31
8.5.1 General . 31
8.5.2 Surface-normal propagation-direction power density into the evaluation
surface, sPD . 31
n+
8.5.3 Total propagating power density into the evaluation surface, sPD . 32
tot+
8.5.4 Total power density directed into the phantom considering near-field
exposure, sPD . 32
mod+
8.6 Software . 33
9 Uncertainty evaluation . 33
9.1 General . 33
9.2 Uncertainty of the sPD and of the mpsPD due to the computational
parameters . 33
9.2.1 Uncertainty contributions due to the computational parameters . 33
9.2.2 Mesh resolution . 34
9.2.3 Absorbing boundary conditions . 35
9.2.4 Power budget . 35
9.2.5 Model truncation . 35
9.2.6 Convergence . 35
9.2.7 Dielectric properties . 36
9.2.8 Lossy conductors . 36
9.3 Uncertainty contribution of the computational representation of the DUT
model . 36
9.4 Uncertainty of the maximum exposure evaluation . 37
9.5 Uncertainty budget . 38
10 Reporting . 39
Annex A (normative) Code verification . 41
A.1 General . 41
A.2 Interpolation and superposition of vector field components . 41
A.3 Computation of the far-field pattern and the radiated power . 43
A.4 Implementation of lossy conductors . 43
A.5 Implementation of anisotropic dielectrics . 46
A.6 Computation of the sPD and psPD . 47
A.6.1 General . 47
A.6.2 Planar surfaces . 49
A.6.3 Non-planar surfaces . 50
A.7 Implementation of the field extrapolation according to the surface
equivalence principle . 52
Annex B (informative) Experimental evaluation of the radiated power . 53
B.1 General . 53
B.2 Direct conducted power measurements . 53
B.3 Radiated power measurement methods . 54
B.4 Information provided by the DUT . 54
Annex C (normative) Maximum-exposure evaluation techniques . 55
C.1 General . 55
C.2 Evaluation of EM fields radiated by each antenna element . 55
C.3 Evaluation of the mpsPD by superposition of individual EM fields . 56
C.3.1 General . 56
C.3.2 Maximization over the entire codebook by exhaustive search . 56
C.3.3 Optimization with fixed total conducted power. 56
– 4 – IEC/IEEE 63195-2:2022 © IEC/IEEE 2022
C.3.4 Optimization with fixed power at each port . 56
Annex D (informative) Examples of the implementation of power density averaging
algorithms . 58
D.1 Example for the evaluation of the psPD on a planar surface . 58
D.1.1 General . 58
D.1.2 Evaluation of the psPD by direct construction of the averaging area . 58
D.1.3 Example for the efficient evaluation of the psPD using an equidistant
mesh on the evaluation surface . 59
D.2 Example for the evaluation of the psPD on a non-planar surface . 60
Annex E (informative) File format for exchange of field data . 62
Annex F (informative) Rationales of the methods applied in IEC/IEEE 63195-1 and this
document . 64
F.1 Frequency range . 64
F.2 Computation of sPD . 64
F.2.1 Application of the Poynting vector for computation of incident power
density . 64
F.2.2 Averaging area . 65
Annex G (informative) Square averaging area on non-planar evaluation surfaces . 66
G.1 General . 66
G.2 Example implementation for the evaluation of the psPD on a non-planar
surface using square-shaped averaging area . 66
Annex H (informative) Validation of the maximum-exposure evaluation techniques . 67
H.1 General . 67
H.2 Validation of the exhaustive search . 67
H.2.1 Validation of the exhaustive search . 67
H.2.2 Validation using reconstruction method . 67
H.2.3 Validation of optimization with fixed total conducted power or with fixed
power at each port . 67
H.2.4 Validation of the maximum-exposure evaluation of measurement results . 67
H.3 Example validation source for maximum-exposure evaluation validation . 68
H.3.1 Description . 68
H.3.2 Positioning. 70
H.3.3 Nominal codebook, uncertainty and conducted power P . 71
R
H.3.4 Target values. 71
Annex I (normative) Supplemental files and their checksums . 73
Bibliography . 74
Figure 1 – Overview of the numerical power density evaluation procedure . 17
Figure 2 – Power reference planes . 22
Figure 3 – Example for configurations of radiating elements as different antenna sub-
arrays on the same DUT . 27
Figure 4 – Flow chart for the evaluation of power density for DUTs with antenna arrays
or sub-arrays as described in 8.2.3 . 28
Figure 5 – Example of the construction of the averaging area within a sphere with fixed
radius according to 8.4 . 31
Figure A.1 – Configuration of three λ/2 dipoles, D , D , and D , for the evaluation of
1 2 3
the interpolation and superposition of the electric field and magnetic field components . 42
Figure A.2 – R320 waveguide . 45
Figure A.3 – Cross section of the R320 waveguide showing the locations of the E
y
components to be recorded . 46
Figure A.4 – S (x,y) computed with Formula (A.4) for the six parameter sets of
i
Table A.6 normalized to their maxima . 49
Figure A.5 – Cross sections of the symmetric quarters of the testing geometries (SAR
Stars) for the benchmarking of the power density averaging algorithm . 51
Figure A.6 – Areas for the computation of the sPD on a cone of the SAR Star . 51
Figure D.1 – Rotated averaging area on the discretized evaluation surface (base
mesh) . 60
Figure D.2 – Reduction of the area of triangles that are partially included in the
averaging sphere . 61
Figure H.1 – Main dimensions of patch array stencil . 69
Figure H.2 – Main dimensions of the validation device, including polypropylene casing . 70
Figure H.3 – Validation device with SAM head in the tilt position . 70
Figure H.4 – Validation device with SAM head in the touch position . 71
Table 1 – Budget of the uncertainty contributions of the computational algorithm for the
validation setup or testing setup . 34
Table 2 – Budget of the uncertainty of the developed model of the DUT . 37
Table 3 – Computational uncertainty budget . 38
Table A.1 – Interpolation and superposition of vector field components; maximum
permissible deviation from the reference results is 10 % . 42
Table A.2 – Computation of P ; maximum permissible deviation from the reference
R
results is 10 % for the radiated power and for the electric field amplitude of the far-
field pattern . 43
Table A.3 – Minimum fine and coarse mesh step for used method . 46
Table A.4 – Results of the evaluation of the computational dispersion characteristics . 46
Table A.5 – Results of the evaluation of the representation of anisotropic dielectrics . 47
Table A.6 – Parameters for the incident power density distribution of Formula (A.4) . 48
Table B.1 – Comparison of the experimental methods for the evaluation of the radiated
power . 53
Table H.1 – Main dimensions for the patch array stencil . 68
Table H.2 – Main dimensions of the validation device . 68
Table H.3 – Target values for validation device with the nominal codebook. 72
Table H.4 – Target values for validation device with infinite codebook . 72
– 6 – IEC/IEEE 63195-2:2022 © IEC/IEEE 2022
INTERNATIONAL ELECTROTECHNICAL COMMISSION
____________
ASSESSMENT OF POWER DENSITY OF HUMAN EXPOSURE TO RADIO
FREQUENCY FIELDS FROM WIRELESS DEVICES IN CLOSE PROXIMITY
TO THE HEAD AND BODY (FREQUENCY RANGE OF 6 GHz TO 300 GHz) –
Part 2: Computational procedure
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IEC/IEEE 63195-2 was prepared by IEC technical committee 106: Methods for the assessment
of electric, magnetic and electromagnetic fields associated with human exposure, in
cooperation with the International Committee on Electromagnetic Safety (ICES) of the IEEE
Standards Association, under the IEC/IEEE Dual Logo Agreement between IEC and IEEE. It is
an International Standard.
This document is published as an IEC/IEEE Dual Logo standard.
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The text of this International Standard is based on the following IEC documents:
Draft Report on voting
106/564/FDIS 106/569/RVD
Full information on the voting for its approval can be found in the report on voting indicated in
the above table.
The language used for the development of this International Standard is English.
This document was drafted in accordance with the rules given in the ISO/IEC Directives, Part 2,
available at www.iec.ch/members_experts/refdocs. The main document types developed by IEC
are described in greater detail at www.iec.ch/standardsdev/publications.
A list of all parts in the IEC/IEEE 63195 series, published under the general title Assessment
of power density of human exposure to radio frequency fields from wireless devices in close
proximity to the head and body, can be found on the IEC website.
The IEC Technical Committee and IEEE Technical Committee have decided that the contents
of this document will remain unchanged until the stability date indicated on the IEC website
under webstore.iec.ch in the data related to the specific document. At this date, the document
will be
• reconfirmed,
• withdrawn,
• replaced by a revised edition, or
• amended.
IMPORTANT – The "colour inside" logo on the cover page of this document indicates that it
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– 8 – IEC/IEEE 63195-2:2022 © IEC/IEEE 2022
INTRODUCTION
This document provides a method to evaluate the human exposure from wireless devices using
computational methods. This document was developed to provide procedures for the numerical
modelling and evaluation of such wireless devices operating close to the head, held in the hand
or in front of the face, mounted on the body or embedded in garments. It applies to individual
transmitters as well as to transmitters operating simultaneously with other transmitters within a
product. The choice of technique, i.e. FDTD or FEM, is optional but can be influenced by the
application. The advantages of computational procedures include the capability to provide
repeatable, non-intrusive methods for determining exposure in or near an object and without
the need for expensive hardware equipment. Device categories covered include but are not
limited to mobile telephones, radio transmitters in personal computers, desktop and laptop
devices, and multi-band and multi-antenna devices. This document specifies:
• requirements on the numerical software (Clause 5);
• model development and validation (Clause 7);
• power density computation and averaging (Clause 8);
• uncertainty evaluation (Clause 9);
• reporting requirements (Clause 10).
To develop this document, IEC Technical Committee 106 (TC 106) and IEEE International
Committee on Electromagnetic Safety (ICES), Technical Committee 34 (TC 34) Subcommittee
1 (SC 1) formed Joint Working Group 11 (JWG 11) on computational methods to assess the
power density of human exposure to radio frequency fields from wireless devices in close
proximity to the head and body.
ASSESSMENT OF POWER DENSITY OF HUMAN EXPOSURE TO RADIO
FREQUENCY FIELDS FROM WIRELESS DEVICES IN CLOSE PROXIMITY
TO THE HEAD AND BODY (FREQUENCY RANGE OF 6 GHz TO 300 GHz) –
Part 2: Computational procedure
1 Scope
This document specifies computational procedures for conservative and reproducible
computations of power density (PD) incident to a human head or body due to radio-
frequency (RF) electromagnetic field (EMF) transmitting devices. The computational
procedures described are finite-difference time-domain (FDTD) and finite element methods
(FEM), which are computational techniques that can be used to determine electromagnetic
quantities by solving Maxwell’s equations within a specified computational uncertainty. The
procedures specified here apply to exposure evaluations for a significant majority of the
population during the use of hand-held and body-worn RF transmitting devices. The methods
apply to devices that can feature single or multiple transmitters or antennas, and that can be
operated with their radiating part or parts at distances up to 200 mm from a human head or
body.
This document can be employed to determine conformity with any applicable maximum PD
requirements of different types of RF transmitting devices used in close proximity to the head
and body, including those combined with other RF transmitting or non-transmitting devices or
accessories (e.g. belt-clip), or embedded in garments. The overall applicable frequency range
of these protocols and procedures is from 6 GHz to 300 GHz.
The RF transmitting device categories covered in this document include but are not limited to
mobile telephones, radio transmitters in personal computers, desktop and laptop devices, and
multi-band and multi-antenna devices.
The procedures of this document do not apply to PD evaluation of electromagnetic fields emitted
or altered by devices or objects intended to be implanted in the body.
NOTE For the evaluation of the combined exposure from simultaneous transmitters operating on frequencies below
6 GHz, the relevant standards for SAR computation are IEC/IEEE 62704-1:2017 and IEC/IEEE 62704-4:2020.
2 Normative references
The following documents are referred to in the text in such a way that some or all of their content
constitutes requirements 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/IEEE 62704-1:2017, Determining the peak spatial-average specific absorption rate (SAR)
in the human body from wireless communications devices, 30 MHz to 6 GHz – Part 1: General
requirements for using the finite difference time-domain (FDTD) method for SAR calculations
IEC/IEEE 62704-4:2020, Determining the peak spatial-average specific absorption rate (SAR)
in the human body from wireless communications devices, 30 MHz to 6 GHz – Part 4: General
requirements for using the finite element method for SAR calculations
– 10 – IEC/IEEE 63195-2:2022 © IEC/IEEE 2022
IEC/IEEE 63195-1:2021 , Assessment of power density of human exposure to radio frequency
fields from wireless devices in close proximity to the head and body (frequency range of 6 GHz
to 300 GHz) – Part 1: Measurement procedure
IEEE Std 145, IEEE Standard for Definitions of Terms for Antennas
3 Terms and definitions
For the purposes of this document, the following terms and definitions apply.
ISO, IEC, and IEEE maintain terminological databases for use in standardization at the following
addresses:
• IEC Electropedia: available at http://www.electropedia.org/
• ISO Online browsing platform: available at http://www.iso.org/obp
• IEEE Dictionary Online: available at http://dictionary.ieee.org
3.1 Exposure metrics and parameters
3.1.1
power density
PD
local power density
function of the complex Poynting vector S at the location r that is integrated over a surface to
compute the sPD
Note 1 to entry: Specifications of power density in terms of the integrands of Formula (4), Formula (5), and
Formula (8) are provided in 8.5. See also rationales provided in Annex F for the PD specifications of 8.5.
Note 2 to entry: The formula used to compute PD can depend on the applicable exposure guidelines or national
regulations.
Note 3 to entry: Power density is also referred to as power flux density.
Note 4 to entry: The associated term incident power density refers to quantity of power per unit area that impinges
on the body surface. The incident power density just outside the body surface is used to establish local exposure
reference levels, which apply at frequencies above 6 GHz in some jurisdictions.
3.1.2
spatial-average power density
sPD
PD (3.1.1) averaged over a surface of area A
av
Note 1 to entry: sPD is a function of the location vector r. It is determined on the evaluation surface, except for the
edges where no averaging area can be constructed.
2 2
Note 2 to entry: Example averaging area sizes specified in exposure limits are 1 cm and/or 4 cm .
___________
To be published.
3.1.3
peak spatial-average power density
psPD
global maximum value of all the sPD (3.1.2) values on the evaluation surface (3.2.2)
Note 1 to entry: psPD is given by Formula (1)
(1)
psPD = max sPD r
{ ( )}
r
where r is a point on the evaluation surface.
Note 2 to entry: Other local maxima (i.e. secondary peak spatial-average power density values) can exist.
3.1.4
maximized peak spatial-average power density
mpsPD
psPD (3.1.3) of the excitation vector (3.3.5) that maximizes its value
3.1.5
Poynting vector
S
vector product of the electric field strength E and the magnetic field strength H of the
electromagnetic field at a given point
Note 1 to entry: The flux of the Poynting vector through a closed surface is equal to the electromagnetic power
passing through this surface.
Note 2 to entry: For a periodic electromagnetic field, the time average of the Poynting vector is a vector the direction
of which, with certain reservations, can be considered as being the direction of propagation of electromagnetic energy
and the magnitude of which can be considered as being the average power flux density.
Note 3 to entry: For a sinusoidal wave of angular frequency ω, the complex Poynting vector is expressed by
Formula (2)
∗
(2)
S EH×
where E and H are phasors and the asterisk denotes the complex conjugate.
Note 4 to entry: The Poynting vector has units of watt per square metre (W/m ).
[SOURCE: IEC 60050-121:2019, 121-11-66 and IEC 60050-705:1995, 705-02-10, modified –
The entries have been combined and rearranged; Note 4 has been added.]
3.1.6
conservative estimate
estimate of the exposure, including uncertainties as specified in this document,
representative of and slightly higher than that expected to occur in the head or body of a
significant majority of the human population during intended use of a wireless transmitting
device
3.2 Spatial, physical, and geometrical parameters associated with exposure metrics
3.2.1
averaging area
A
av
nominal size of the area used for computing sPD (3.1.2)
Note 1 to entry: On a planar evaluation surface, sPD is computed as the ratio of power density (3.1.1) integrated
over the averaging area A . On a non-planar evaluation surface, the averaging area indicates the dimensions of the
av
projection of the integration area of the power density on a planar surface.
=
– 12 – IEC/IEEE 63195-2:2022 © IEC/IEEE 2022
Note 2 to entry: See details on averaging in 8.4.
3.2.2
evaluation surface
virtual surface for the evaluation of the spatial-average power density (sPD) emitted by a DUT
Note 1 to entry: Typical evaluation surfaces that can be applied in this document are the inner shell of the SAM
phantom with an added pinna, or a planar surface with finite or infinite extension.
Note 2 to entry: The evaluation of the psPD (3.1.3) on the evaluation surface should yield a conservative estimate
(3.1.6) of the exposure.
Note 3 to entry: In practice, an evaluation surface can be different from a measurement surface or area.
3.2.3
near-field
region encompassed by the reactive near-field and the radiative near-field
Note 1 to entry: See also 3.2.5 and 3.2.4 for definitions of reactive near-field and radiative near-field, respectively.
3.2.4
radiative near-field
region of space between the reactive near-field and the far-field, wherein the predominant
components of the electromagnetic field are those that represent a propagation of energy, and
wherein the angular field distribution is dependent upon the distance from the antenna
Note 1 to entry: In the radiative near-field,
...
기사 제목: IEC/IEEE 63195-2:2022 - 머리와 몸 부근에서의 무선 기기로부터 인체 노출에 대한 라디오 주파수 필드의 전력 밀도 평가 (6 GHz에서 300 GHz의 주파수 범위) - 파트 2: 계산 절차 기사 내용: IEC/IEEE 63195-2:2022는 보수적이고 재현 가능한 전력 밀도 (PD) 계산을 위한 계산 절차를 명시합니다. 이 계산 절차는 라디오 주파수 (RF) 전자기장 (EMF) 송신 기기에 의해 인체 머리나 몸에 들어오는 전력 밀도 (PD)를 결정하는 데 사용할 수 있는 계산 기술인 유한차이 시간 영역법 (FDTD)과 유한요소법 (FEM)을 기술합니다. 여기서 기술된 계산 절차는 손에 들거나 몸에 착용하는 RF 송신 기기를 사용하는 인구의 대다수에게 노출 평가에 적용됩니다. 이 방법은 단일 또는 다중 송신기 또는 안테나를 갖출 수 있는 기기 및 인체 머리나 몸과 최대 200mm 거리에서 작동할 수 있는 기기에 적용됩니다. 이 문서는 머리와 몸에 근접하게 사용되는 다른 종류의 RF 송신 기기의 모든 적용 가능한 최대 PD 요구 사항을 확인하는 데 사용할 수 있으며, 이에는 다른 RF 송신 또는 비송신 기기 또는 부속품 (예: 벨트 클립)과 결합된 기기나 의류에 내장된 경우도 포함됩니다. 이 프로토콜과 절차의 적용 주파수 범위는 6 GHz에서 300 GHz까지이다. 이 문서에서 다루는 RF 송신 기기 범주에는 모바일 전화, 개인용 컴퓨터의 라디오 송신기, 데스크톱 및 노트북 장치, 다중 대역 및 다중 안테나 기기 등이 포함되지만 이에 국한되지 않습니다. 이 문서의 절차는 몸 내에 삽입되도록 설계된 장치 또는 물체에서 방출되거나 변경된 elektromagnetic fields에 대한 PD 평가에는 적용되지 않습니다. 참고: 6 GHz 미만 주파수에서 동시 송신기로부터의 병합된 노출 평가에 대해서는 SAR 계산을 위한 관련 표준인 IEC/IEEE 62704-1:2017 및 IEC/IEEE 62704-4:2020을 사용해야 합니다. 이 게시물은 IEC/IEEE 이중 로고 표준으로 출판되었습니다.
記事タイトル:IEC/IEEE 63195-2:2022 - 頭部および体に近接した位置での無線デバイスからの人体への電磁波曝露の電力密度の評価(6 GHzから300 GHzの周波数範囲)- パート2:計算手順 記事内容:IEC/IEEE 63195-2:2022は、無線デバイスからの頭部または体への電磁波(EMF)による人体への電力密度(PD)の保守的で再現可能な計算手順を指定しています。説明されている計算手順は、有限差分時間領域法(FDTD)および有限要素法(FEM)であり、マクスウェルの方程式を解くことによって電磁量を正確に決定するための計算手法です。これらの手順は、手持ちや体に装着した無線デバイスの使用中における人口の大部分の曝露評価に適用されます。この手法は、シングルまたはマルチトランスミッターまたはアンテナを搭載したデバイスに適用可能であり、その放射部の距離が頭部または体から最大200 mm以内で運用されることがあります。 この文書は、頭部および体に近接した位置で使用されるさまざまな種類の無線デバイスの適用可能な最大PD要件に対する準拠性を判定するために使用できます。これには、他の無線送信または非送信デバイスやアクセサリ(例えば、ベルトクリップ)と組み合わさったデバイスや衣類に埋め込まれたデバイスなどが含まれます。これらのプロトコルと手順の適用可能な周波数範囲は6 GHzから300 GHzです。 この文書でカバーされるRF送信デバイスのカテゴリには、携帯電話、パーソナルコンピュータのラジオ送信機、デスクトップおよびノートパソコンデバイス、およびマルチバンドおよびマルチアンテナデバイスなどが含まれますが、これに限定されません。 この文書の手順は、体内に埋め込まれるデバイスやオブジェクトから放射または変更される電磁場のPD評価には適用されません。 6 GHz以下の周波数での複数の送信機からの複合的な曝露の評価のためには、特定吸収率(SAR)計算の関連する標準であるIEC/IEEE 62704-1:2017およびIEC/IEEE 62704-4:2020を使用する必要があります。 この出版物はIEC/IEEEデュアルロゴ規格として公開されています。
기사 제목: IEC/IEEE 63195-2:2022 - 머리와 몸과의 근접한 거리에서 무선 기기로부터 전파 강도에 대한 인체 노출 평가 (6 GHz에서 300 GHz의 주파수 범위) - 파트. 2: 계산 절차 기사 내용: IEC/IEEE 63195-2:2022는 무선 주파수(RF) 전자기장(EMF) 송신 장치로 인한 인체 머리 또는 몸에 입사하는 파워 밀도(PD)를 보수적이고 재현 가능한 계산 절차를 명시한다. 여기서 기술된 계산 절차는 유한 차분 시간 도메인(FDTD)과 유한 요소 메서드(FEM)로 구성되어 있으며, 메솔라의 방정식을 푸는 것을 통해 전자기적인 수량을 정확하게 결정할 수 있는 계산 기술이다. 이 문서는 손에 들고 사용되거나 몸에 착용된 RF 송신 장치의 대부분의 인구를 위한 노출 평가에 적용된다. 이 방법은 단일 또는 다중 송신기 또는 안테나를 갖춘 장치에 적용되며, 인체 머리 또는 몸과의 최대 거리가 200mm 이내에서 운용될 수 있다. 이 문서는 머리와 몸과의 근접한 거리에서 사용되는 다양한 유형의 RF 송신 장치의 최대 PD 요구 사항에 대한 준수 여부를 결정하는 데 사용될 수 있으며, 이에는 다른 RF 송신 또는 비송신 장치 또는 액세서리(예: 벨트 클립)와 결합된 장치 또는 의류에 내장된 장치도 포함된다. 이러한 프로토콜과 절차의 전반적인 적용 가능한 주파수 범위는 6 GHz에서 300 GHz이다. 이 문서에서 다루는 RF 송신 장치 카테고리는 휴대 전화, 개인 컴퓨터의 라디오 송신기, 데스크톱 및 노트북 장치, 다중 밴드 및 다중 안테나 장치 등이 포함되지만 이에 국한되지는 않는다. 이 문서의 절차는 몸에 삽입되는 장치나 물체에 의해 방출되거나 변조되는 전자기장의 PD 평가에 적용되지 않는다. 참고로 6 GHz 이하 주파수에서 동시 송신기로부터의 복합 노출을 평가하기 위해 SAR 계산을 위한 관련 표준은 IEC/IEEE 62704-1:2017 및 IEC/IEEE 62704-4:2020이다. 이 게시물은 IEC/IEEE 이중 로고 표준으로 게시된다.
The article discusses the IEC/IEEE 63195-2:2022 standard, which provides computational procedures for assessing the power density (PD) of human exposure to radio frequency (RF) fields from wireless devices in close proximity to the head and body. The standard describes two computational techniques, finite-difference time-domain (FDTD) and finite element methods (FEM), which can be used to determine electromagnetic quantities by solving Maxwell's equations. These procedures are applicable to hand-held and body-worn RF transmitting devices that can be operated with their radiating parts up to 200 mm away from a human head or body. The standard can be used to assess compliance with maximum PD requirements for different types of RF transmitting devices used near the head and body, including those combined with other devices or accessories. The frequency range covered by these procedures is from 6 GHz to 300 GHz. The standard does not apply to PD assessment of electromagnetic fields emitted or altered by devices intended to be implanted in the body. For assessing combined exposure from simultaneous transmitters at frequencies below 6 GHz, other relevant standards should be used. The publication is published as an IEC/IEEE Dual Logo standard.
The article discusses the IEC/IEEE 63195-2:2022 standard, which provides computational procedures for determining the power density of human exposure to radio-frequency fields from wireless devices. The standard includes finite-difference time-domain and finite element methods for accurately calculating electromagnetic quantities based on solving Maxwell's equations. These procedures are applicable to handheld and body-worn devices with single or multiple transmitters or antennas, operating within 200 mm of the head or body. The standard can be used to assess compliance with maximum power density requirements for different types of devices operating in the frequency range of 6 GHz to 300 GHz. However, it does not cover devices implanted in the body. For assessing combined exposure from multiple transmitters below 6 GHz, other relevant standards for specific absorption rate (SAR) computation should be used. This publication is released as an IEC/IEEE Dual Logo standard.
記事タイトル: IEC/IEEE 63195-2:2022 - 頭部と体に近接したワイヤレスデバイスからの人体への電磁波曝露のパワー密度評価(6 GHzから300 GHzの周波数範囲)- パート2: 計算手順 記事内容: IEC/IEEE 63195-2:2022は、ラジオ周波数(RF)電磁界(EMF)送信デバイスによる人体の頭部または体への結節点波(PD)の積体評価のための計算手順を指定しています。ここで説明されている計算手順は、Maxwell方程式を解くことによって電磁量を決定するために使用できる有限差分時間領域法(FDTD)および有限要素法(FEM)という計算技術です。説明されている手順は、手持ちや体に装着されたRF送信デバイスの使用中に一般的に安全確保が必要な人口の大部分に適用されます。これらの手法は、単一または複数のトランスミッターやアンテナを備えたデバイスにも適用され、人体の頭部または体から最大200 mm離れた位置で動作することができます。 本文書は、頭部と体に近接して使用されるさまざまなタイプのRF送信デバイスの適用可能な最大PD要件の遵守を確認するために利用することができます。これには他のRF送信または非送信デバイスやアクセサリー(例:ベルトクリップ)と組み合わされたデバイスや衣類に埋め込まれたデバイスも含まれます。これらの手順とプロトコルの適用可能な周波数範囲は6 GHzから300 GHzです。 本文書でカバーされているRF送信デバイスのカテゴリには、モバイル電話、パーソナルコンピュータのラジオトランスミッター、デスクトップおよびノートパソコンデバイス、マルチバンドおよびマルチアンテナデバイスなどが含まれます。 本文書の手順は、体内に埋め込まれることを意図したデバイスやオブジェクトによって発生または変異される電磁場のPD評価には適用されません。 6 GHz未満の周波数で同時送信機からの結合曝露の評価の場合は、関連するSAR計算のための規格であるIEC/IEEE 62704-1:2017およびIEC/IEEE 62704-4:2020を使用する必要があります。 この記事は、IEC/IEEEデュアルロゴ規格として公開されています。










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