Abstract
In March 2020, the International Commission on Non-Ionizing Radiation Protection (ICNIRP) released its new guidelines () on the limitation of radio frequency (RF) electromagnetic fields (EMF) exposure in the frequency range 100 kHz–300 GHz. These have taken several years to develop and include the review of the latest scientific literature. Most countries worldwide currently apply the RF-EMF exposure limits provided in the guidelines and are expected to align their regulations according to the recently revised limits. In this paper, the implications of the guidelines on the RF-EMF compliance of base stations (BSs) for mobile communications are analyzed in detail. The study covers different types of BS products, from low-power small cells to macro cell equipment, operating within different frequency bands and of relevance for 2G to 5G mobile technologies. A direct comparison of the BS RF-EMF exclusion zones (or compliance boundaries), when the and the limits are applied, is provided. Since existing and future mobile equipment infrastructure is likely to be required to comply with the guidelines, the paper provides useful information to mobile equipment manufacturers, mobile operators, standardization bodies and regulators.
Introduction
On March 11, 2020, ICNIRP released new guidelines, referred in this report as “,” for exposure to RF EMF in the frequency range 100 kHz–300 GHz (). As a consequence, many countries worldwide are expected to update their radio wave standards based on the new ICNIRP international guidelines (e.g., ). Several national regulations are likely to change from the previous version of the ICNIRP guidelines (), referred in this report as “,” to the new ones. While the limits have been confirmed to be protective for current technologies (including 5G), some changes have been introduced making the guidelines “future-proofed” (). A summary of the main differences between and the previous guidelines is provided by ICNIRP ().
Mobile equipment, including BSs and mobile devices, need to comply with RF EMF exposure limits, such as those recommended by ICNIRP. These exposure limits are set far below the lowest level required to cause adverse health effects which are related to induced heating in the body. The guidelines are technology independent and apply equally to all existing mobile technologies (from 2G to 5G) within the specified frequency range. Several studies have analyzed the implications that the international exposure guidelines have on the design, operation, and deployment of mobile equipment. For instance (), derived an estimate of the maximum transmit power based on the numerical model of canonical antennas operating in close proximity of the body (). Conducted a systematic investigation of the allowed output power and maximum equivalent isotropic radiated power (EIRP) of array antennas operating at frequencies above 10 GHz. These studies were conducted before the publication of the revised limits, and only a single publication addressed the performance of portable devices (e.g., mobile phones) when complying with (). To date, and to the knowledge of the authors, no study evaluating the implications of EMF compliance with for BSs exists.
EMF compliance for BSs typically involves establishing the so-called compliance boundaries or exclusion zones, i.e., the volume surrounding the base station antenna (or the base station itself when radio transmitters and antenna are tightly integrated) outside of which EMF exposure is below the limits. Therefore, in this work, the implications of are addressed by establishing the compliance boundaries for several BSs, representative of different technologies, installation scenarios, and frequency bands. Results are provided for conventional multi-column passive antennas as well as massive MIMO (mMIMO) antennas, which are becoming more common with the deployment of 5G. Low-power BSs typically used for indoor coverage are also addressed. Considerations are made for different frequencies, within relevant mobile communication bands below as well as above 6 GHz.
A brief summary of the limits is given in Section 2. The methodology used to assess the BS compliance boundaries for different types of antennas and BS products is provided in Section 3. Results are presented in Section 4 while the implications of the limits for brief exposure are specifically addressed in Section 5. Some reflections about the results are given in Section 6. Final conclusions are drawn in Section 7.
Summary of the RF-EMF Limits Specified by ICNIRP 2020
ICNIRP RF EMF exposure limits are given in terms of basic restrictions, which relate to physical quantities inside the body, and in terms of reference levels, which are external field quantities derived from the basic restrictions. The reference levels provide a more practical mean of assessing compliance in most situations. Basic restrictions and reference levels are specified for whole-body and local exposure. A summary of the basic restrictions applicable for the general public and for frequencies above 400 MHz, as given by , is provided in Annex A, Supplementary Table A1 (as supplementary material). The corresponding reference levels are presented in Supplementary Table A2.
also provides basic restrictions and reference levels applicable for “brief exposure,” i.e., for “exposure from any pulse, group of pulses, or subgroup of pulses in a train, as well as from the summation of exposures (including non-pulsed EMFs), delivered in t seconds (t < 360 s)”. Such limits are only applicable for local exposure (Supplementary Table A3). For convenience, a brief summary of the limits is included in Annex A (as supplementary material) but the tables provided in the guidelines (), should be used as a more exhaustive and rigorous reference.
In Section 3, the compliance boundaries (exclusion zones) for several BSs are determined according to and compared to those obtained when using , for which the applicable limits are summarized in Supplementary Tables A4, A5.
EMF compliance for BSs is typically assessed by means of the reference levels since the usage of the basic restrictions is often unpractical (
). The main differences in the reference levels specified by
compared with
are listed below and summarized in
Table 1(only frequencies above 400 MHz are considered):
• Below 10 GHz, incident power density and field strength limit values applicable for whole-body exposure (i.e., spatially averaged over an area corresponding to the body surface) are the same as those provided by . does not provide specific reference levels for local exposure but the whole-body reference levels can be applied as spatial-peak values, when it is necessary to assess compliance for partial-body exposure. introduces additional reference levels for local exposure that are higher than those applicable for whole-body (e.g., of a factor of 4 between 2 and 6 GHz). It follows that the reference levels for local exposure in are larger than those used according to .
• Above 10 GHz, specifies the limit in terms of incident power density averaged over 20 cm2. The same power density limit values are provided by for whole-body exposure reference levels and are intended to be averaged over an area corresponding to the whole-body surface (much larger than 20 cm2). At the same time, reference levels for local exposure are introduced and are to be averaged over a smaller area such as 4 cm2 (above 30 GHz, averaging areas of both 4 and 1 cm2 apply; for the latter, the corresponding power density limit values have to be doubled.) The local incident power density limits are higher than the whole-body ones also in this frequency range (e.g., about a factor of 3 at 30 GHz).
• The averaging time applicable for whole-body exposure according to is extended to 30 min in the entire frequency range. The corresponding time for local exposure is 6 min. averaging time is dependent on frequency.
• In the reactive near-field region and at frequencies above 2 GHz, the reference levels cannot be used, and compliance with guidelines needs to be assessed by means of the basic restrictions.
TABLE 1
| ICNIRP (1998) | ICNIRP 2020 | |
|---|---|---|
| Whole-body exposure below 10 GHz | The same field strength and incident power density limits apply for and . Above 2 GHz uses only incident power density as reference levels (electric and magnetic field strength limits are not specified) | |
| Whole-body exposure above 10 GHz | The same incident power density limits apply but greater specification on the applicable averaging area is given by | |
| According to the basic restrictions, incident power density is to be averaged over any 20 cm2 of the exposed area | According to , incident power density is to be averaged over an area corresponding to the whole-body surface | |
| Local exposure | No specific reference levels for local exposure | Specific reference levels for local exposure that are larger than those for whole-body exposure are provided by ICNIRP 2020 |
| Compliance for local exposure when using reference levels is established applying the whole-body reference levels as spatial-peak values | ||
| Averaging time for whole-body exposure | 6 min or less depending on frequency | Fixed to 30 min up to 300 GHz |
| Averaging time for local exposure | 6 min or less depending on frequency | Fixed to 6 min up to 300 GHz |
| Applicability of reference levels in the reactive near-field region | The contribution of the electric and magnetic fields needs to be considered separately | Above 2 GHz, the reference levels cannot be applied (assessments must be based on the basic restrictions) |
Comparison of the reference levels applicable to the general public as specified by and at frequencies above 400 MHz. Brief exposure limits applicable for intervals below 6 min are discussed separately in Section 5.
Basic restrictions may be used to assess EMF compliance for BS products with very low power, which are addressed separately in Section 4.3. New local energy limits applicable for intervals of less than 6 min have also been specified by and are discussed in detail in Section 5.
The guidelines, as before, differentiate between occupationally exposed individuals and general public. The limits for occupational exposure can be derived from those applicable to the general public by scaling them with a factor of 5.
Methods
Compliance Boundary Evaluation
The BS compliance boundary is characterized by a complex shape (iso-surface), which depends on the radiation characteristics of the antenna. More practical compliance boundaries can be used by enclosing the iso-surface with volumes of simpler shape, which are also easier to communicate () and therefore to implement when installing a BS. In this paper, a box-shaped compliance boundary is used, characterized by its width, height, and front compliance distance, as depicted in Figure 1. While the fit to the iso-surface compliance boundary is made as tight as possible, the box might overestimate the compliance distance is some directions. Outside of this box, the RF exposure is below the limits.
FIGURE 1
Exposure assessment standards, such as (), define RF exposure assessment methodologies applicable for BSs, including measurements, advanced numerical methods, and basic computation techniques. Such standards also provide criteria to identify the most suitable evaluation method depending on the source characteristics and on the purpose of the assessment (e.g., product compliance, product installation compliance, or in-situ assessments). Calculations using the spherical formula is the most common and standard way to assess the compliance boundary of base station antennas:where , and denote the incident power density (W/m2), the accepted power (W), the antenna gain (linear ratio), the distance from the antenna (m), and the angular variables in a spherical coordinate system, respectively. This formula assumes free-space condition, which is a reasonable assumption when evaluating exposure at distances corresponding to the compliance boundary (e.g., shorter than 30 m). Under such condition, power density predicted by the formula is deemed to be accurate ().
The antenna gain values used in this paper are provided, on the horizontal and vertical cuts (see Section 3.2), directly by the antenna manufacturers, based on measurements of the radiation pattern. For mMIMO products, characterized by several antenna ports, the traffic beams are steered in different directions, depending on the location of the users requesting service. Therefore, in the equation above corresponds to the envelope of the antenna gain for all possible beams (). For multi-column conventional (non-mMIMO) antennas, the antenna gain is typically provided by the manufacturers for each antenna port. In this paper, power density for ports corresponding to the same nominal polarizations (denoted ±45°) is combined by summing the fields in a correlated way. By means of this conservative approach, the field transmitted from antenna ports with the same nominal polarization is assumed to be in-phase. In contrast, exposure from antenna ports with orthogonal nominal polarizations (±45°) are summed in an uncorrelated manner. For instance, for two antenna columns denoted 1 and 2 (each column has two orthogonal ports, i.e., four antenna ports in total), the total power density as estimated by the spherical formula is given by:
The iso-surface compliance boundaries for the selected BS antennas are obtained by solving the following equation for :where (W/m2) corresponds to the reference level limit values provided in Annex A. The box-shaped compliance boundary is then derived from the smallest box enclosing this surface.
A MATLAB-based Ericsson internal software tool was used to calculate power density according to expressions 1) and 2) and to plot the corresponding compliance boundary (3). The tool provides an interface for users to select antenna pattern files and insert the parameters needed to calculate the power density, such as the antenna accepted power.
While for , the compliance boundaries are obtained by means of expression 3) using the reference levels in Supplementary Table A5 as spatial peak values, provides specific reference levels for both local and whole-body exposure (both to be met). Whole-body incident power density is therefore to be averaged over an area corresponding to the whole-body surface. While ICNIRP does not recommend a specific size of this surface, in this work averaging is performed over a line, corresponding to the height of the child whole-body phantom specified in IEC 62232, i.e., 0.96 m. The average power density, at a generic point is therefore obtained as:
IEC 62232 () provides recommendation on different averaging schemes for whole-body exposure, including vertical lines and cross-sectional areas. Among these, for a fixed body height, averaging over a line provides conservative results with respect to other alternatives. In addition, while it is reasonable to conduct averaging assuming the body height oriented parallel to the antenna axes (i.e., along z), the orientation of the body width, and therefore the orientation of the cross-sectional surface, might be arbitrary and difficult to set (any direction on the xy-plane could be justifiable).
Selected BS Products
The relevant characteristics of the BS products or BS antennas selected for this study are summarized in Table 2. Antennas are chosen to cover a wide range of frequencies and parameters (in terms of dimensions, gain, half power beamwidth, etc.) relevant for mobile technologies, from 2G to 5G. The antenna gain values in the horizontal cut and vertical cut are provided by the manufacturers (based on measurements). The gain at any angle is subsequently extrapolated, based on the following classical approximation:
TABLE 2
| Antenna/product | Selected frequency (MHz) | Type | Dimensions (m) Height x width x depth | Peak gain (dBi) at the selected frequency1 |
|---|---|---|---|---|
| Comba ODI-065R17M | 728 | 2 ports (1 column, X-polarized) | 2.5 × 0.3 × 0.12 | 16 |
| Comba ODI2-065R17M | 943 | 4 ports (2 columns, X-polarized) | 2.5 × 0.3 × 0.12 | 17 |
| Ericsson Radio 4402 | 1805 | 4 ports (integrated antenna) | 0.45 × 0.20 × 0.13 | 9 |
| CommScope T4-90A-R1-V2 | 2,300 | 8 ports (4 columns, X-polarized) | 1.61 × 0.31 × 0.12 | 17 |
| Ericsson Radio 4402 | 2,690 | 4 ports (integrated antenna) | 0.45 × 0.20 × 0.13 | 11 |
| Ericsson AIR 3236 | 3,400 | Massive MIMO integrated antenna (32 ports) | 0.77 × 0.40 × 0.19 | 24 |
| Ericsson AIR 6449 | 3,600 | Massive MIMO integrated antenna (64 ports) | 0.78 × 0.40 × 0.27 | 25 |
| Comba ODSR-090R16U02Q | 3,600 | 8 ports (4 columns, X-polarized) | 0.9 × 0.26 × 0.12 | 16 |
| Ericsson AIR 1281 | 28,000 | Massive MIMO integrated antenna (24 × 8 ports) | 0.29 × 0.2 × 0.14 | 29 |
| Ericsson Street Macro 6701 | 38,500 | Massive MIMO integrated antenna (24 × 8 ports) | 0.51 × 0.2 × 0.12 | 29 |
Characteristics of the selected BS antennas or BS products (for integrated antennas).
For multi-column conventional (non-mMIMO) antennas, the peak gain is provided for the single port. For mMIMO, the peak gain is obtained from the envelope of the radiation pattern for all possible beams. The values are rounded to the nearest integer.
For BS operating below 6 GHz, the compliance boundaries are determined for a time-averaged input power of 5, 10, 40, 100, 200, and 250 W. Such power levels are selected to span over a wide range of installation scenarios but might differ from what is configurable in reality by the BS. For instance, the Ericsson Radio 4402 is a micro BS product that can be set to operate at power levels up to 20 W and the actual maximum time-averaged transmitted power levels () for Ericsson mMIMO products AIR 3236 and AIR 6449 are up to 80 W. Since the objective of this work is to study the implications of the updated EMF limits rather than to determine the EMF compliance distance for specific products, the broad choice of frequencies, antenna types, and power levels allows to draw general conclusions on the impact of the guidelines on EMF compliance of BSs. The same consideration can be made with regard to the approximation in Eq. 5, which assumes the antenna gain in elevation to be independent of the azimuth angle; although slightly more accurate reconstruction methods of the 3D gain from the radiation pattern on the horizontal and vertical cuts have been proposed, e.g., (), they are unnecessary for the purpose of this study.
BSs operating at 28 and 38.5 GHz are characterized by power levels that are much lower than what are typically supported for “low-band” and “mid-band” BSs (e.g. for the selected BS products, the maximum configurable power is currently 1 W). The compliance boundaries for the “high-band” BS products are therefore determined for 100 mW, 200 mW, 400 mW, 1 W, 2 W, and 5 W.
Results
Micro and Macro BS Operating Below 6 GHz
An example of an iso-surface compliance boundary obtained according to the procedure described in Section 3 for limits is plotted in Figure 2 for the Ericsson AIR 3236, determined from the radiation pattern envelope of the and for a power level of 40 W. The enclosing box-shaped compliance boundary is also visible in the same figure from a picture of the vertical cut (the box is always centered around the antenna in the z direction so the height of the box is conservatively chosen to be equal above and below the antenna).
FIGURE 2
The compliance boundary box dimensions (enclosing the iso-surface) for each of the listed BS antennas operating below 6 GHz are provided in Figures 3–5, for the front, width, and height, respectively. The pale-blue bars correspond to the dimensions obtained according to , while the corresponding distances to comply with (including both whole-body and local exposure) are in orange. Six bars for each BS antenna are plotted corresponding to power levels ranging from 5 to 250 W.
FIGURE 3
FIGURE 4

Widths of the compliance boundary box for the selected BS antennas (for frequencies below 6 GHz) obtained by applying
FIGURE 5

Heights of the compliance boundary box for the selected BS antennas (for frequencies below 6 GHz) obtained by applying
Figures 3–5 clearly indicate that the compliance boundaries based on
Overall, the difference in the compliance boundaries between
The compliance boundary box is determined to always enclose the antenna size (or the BS for radio products with integrated antenna(s)). The cases in Figure 5 characterized by “Height” which remains constant with power, correspond to configurations whose exposure is below the limits within the antenna length. Moreover, it must be considered that the pointwise distribution of calculated with expression (4), identifies whole-body exposure at the center of the averaging line. Therefore, the RF EMF exposure of a person with part of the body within the compliance boundary iso-surface determined through (Figure 6) would still be below the whole-body reference levels. The “Height” of the box, determined by means of is thus reduced by the averaging length (96 cm), in order to obtain compliance boundaries defined consistently (for whole-body as well as for local exposure) as the region outside which the exposure limit is not exceeded by any part of the body. In the far field where the power density is expected to be relatively uniform over the averaging line, the compliance boundary height, obtained by applying
FIGURE 6

Sketch of the compliance boundary height determined when applying
Micro and Macro BS Operating at Frequencies Above 6 GHz
Compliance boundaries are determined for the selected high-frequency BSs according to the method described in Section 3. However, since
The front compliance distances are shown in Figure 7. The compliance distance determined according to
FIGURE 7

Dimension of the compliance boundary box in the front for the selected BS products (for frequencies above 6 GHz) obtained applying
Low Power BS
For low-power base stations (e.g. below 5 W) operating below 6 GHz, the EMF compliance distance is generally assessed by means of the basic restrictions; a detailed example of a compliance assessment of a local area BS product based on SAR is given in (
Above 6 GHz, within the millimeter wave bands, mMIMO BSs currently operate at power levels well below 5 W but the maximum EIRP is comparable to that of macro or micro products due to the use of antenna arrays characterized by a large aperture. Implications of
FIGURE 8

Front compliance distance (≥5 mm) for 2 × 2 and 4 × 4 antenna arrays at 40 GHz as function of the power when applying
Time Averaging and Brief Exposure Limits
The implications of
By dividing the energy limits on brief exposure of Supplementary Table A3 by the corresponding time interval t, the energy limits can be expressed in terms of time-averaged power over any interval t < 6 min and can be directly compared with the steady state (energy rate) limit values of Supplementary Tables A1, A2. The curve in Figure 9 is normalized to the value obtained for t approaching 6 min (t→360 s). The relative function obtained is the same at any frequency for which the brief exposure limits apply and follows the same trend for both basic restrictions and reference levels. It should be noticed that the local exposure limits (both reference levels and basic restrictions), time-averaged over 6 min, and the brief exposure limits when t→360 s are equivalent. The absolute values for the brief exposure limits can, therefore, be obtained by scaling the curve in Figure 9 with the limits presented in Supplementary Tables A1, A2 for “steady-state” local exposure.
FIGURE 9

Limit for “brief exposure” (t < 6 min), see Supplementary Table A3, divided by the corresponding time interval t and normalized with the value obtained for t approaching 6 min. For visualization purposes, the curve is plotted for t > 1 s. For shorter t, the limits for brief exposure increase (the corresponding normalized value for t = 1 ms is about 18,567).
When the compliance boundary of the BS is determined assuming constant peak power transmission (in every direction for BS implementing beamforming), the brief exposure limits are not relevant. Under this condition, compliance with the 6-min time-averaged local exposure limits ensures compliance with the guidelines on brief exposure. Figure 9 also indicates that only the root-mean-square (rms) power is relevant for assessing EMF compliance since the oscillations of the instantaneous power around the rms value need to be exceptionally large to exceed the energy limits. For this reason, the effect of modulation of signals transmitted by BSs are irrelevant to the objective of assessing compliance with the limits for brief intervals. For instance, while the maximum realistic peak-to-average power ratio of NR and LTE BS signals is about 10 dB, the power over a symbol time (e.g. 36 µs) required to exceed the brief exposure limits, when complying with the 6-min time-averaged limits, has to be about 500,000 times (57 dB) larger, which will never occur.
BS products that make use of beamforming can be assessed according to the “actual” maximum transmitted power, , according to the requirements of IEC 62232. While the “theoretical” maximum transmitted power unrealistically assumes constant peak power transmission for any possible beam, the actual maximum is obtained by taking into consideration that the energy is spatially spread in different directions to serve the users. The actual maximum transmitted power, therefore, is only a fraction of the theoretical maximum (
For BS transmitting with an actual time-averaged power level, , and the whole-body exposure complying with the time-averaged reference levels, , as shown in Supplementary Table A2, the maximum possible incident energy density (J/m2) when the BS is transmitting at the peak power level during the time duration is:where is the averaging time for whole-body exposure (i.e., 30 min). To meet the limits on brief exposure, as given in Supplementary Table A3, the maximum energy in the pulse, as allowed by the time-averaged reference levels, should also satisfy the following conditions for any time t:
From expression (8), it is possible to derive the lowest PRF value (PRFmin) for which compliance with the whole-body time-averaged reference levels of Supplementary Table A2 inherently ensures compliance with the limits on brief exposure (Supplementary Table A3). PRFmin is provided for some frequencies in Figure 10 as a function of the pulse duration.
FIGURE 10

PRFmin as function of the pulse duration for some selected frequencies. For PRF values equal to or above PRFmin, compliance with the whole-body time-averaged limits (over 30 min) inherently ensures compliance with the limits on brief exposure.
While PRFmin depends on the pulse duration, Figure 10 shows that for any possible pulse at frequencies between 2 and 6 GHz, compliance with the incident power density reference levels applicable for whole-body exposure, time-averaged over 30 min, ensures compliance with the limits on energy density (for brief exposure) for PRF equal to or larger than 0.25. The corresponding PRF values for 700 MHz, 28 and 39 GHz are 0.22, 0.33, and 0.35, respectively.
Figure 10 is limited to pulse durations of 6 min since brief exposure limits are limited within this time interval. As the averaging time applicable to whole-body exposure is 30 min, pulses of longer durations are possible but the energy delivered within any integration interval between 0 and 360 s is still inherently compliant with , in Supplementary Table A3 for PRF ≥ PRFmin.
Note that PRFmin is determined by directly comparing the maximum possible energy in a pulse, as allowed by the whole-body reference levels, with the energy density limits intended for local exposure, without considering the difference in the applicable spatial averaging areas. Since for macro base stations (see Sections 4.1, 4.2), power density at the compliance distance is typically uniform over the whole-body surface (or line), the effect of spatial averaging can be considered negligible. At short distances from a BS, where the field distribution is more complex, or in general if the power density is not uniform over the averaging area, the criteria on PRFmin are still applicable, if compliance with the whole-body reference levels is determined without applying spatial averaging over the whole-body surface.
When applying the basic restrictions below 6 GHz, the ratio between whole-body SAR (SARwb) and local SAR (over a 10 g mass, SARlocal) normalized to their respective limits (i.e., the exposure ratios) provides additional insights to study the relevance of the brief exposure limits on EMF compliance for BS. For this purpose, the ratiois plotted in Figure 11 as the function of the separation distance for three BS models, one at 2.6 GHz and two at 3.5 GHz. The simulated BSs correspond to two mMIMO products characterized by an array of 96 dipoles with 45-degree slant for both simulated frequencies and 64 patch arrays (8 × 8) at 3.5 GHz. SAR is assessed in the box-shaped child phantom specified by IEC 62232 (0.96 m × 0.233 m × 0.15 m) using CST Studio Suite. The antenna model is placed in parallel with the phantom, and their centers are aligned. For separation distances below 1.5 m, in order to accurately characterize the possible interactions between the antenna and the phantom, full-wave simulations based on the Finite Integration Technique (FIT) are conducted. At larger distances, a hybridization of FIT and Method of Moments (MoM) is used to reduce the simulation time, similarly to the procedure described in (
FIGURE 11

Ratio between peak-spatial localized SAR (SARlocal) and whole-body SAR (SARwb) normalized to their respective limits, as a function of the separation distance for mMIMO BS antennas at 2.6 and 3.5 GHz.
PRFmin (e.g., 0.25 between 2 and 6 GHz) values are determined for the extreme case of a BS delivering the highest possible energy in any time interval, when subject to the limit values applicable for whole-body exposure. Such a condition is implausible, since it implies that the BS transmits at peak power continuously for 6 minutes. For mMIMO products this is even more unlikely because, over time, the energy will be spread over different beams. Therefore, in realistic scenarios, compliance with the brief exposure limits is met when complying with the limits for whole-body exposure for PRFs much smaller than PRFmin. As described in (
When assessing the BS compliance boundary according to the actual maximum transmit power, the availability of software features, supporting the BS scheduler and able to monitor and/or control the time-averaged transmit power during operation, might be required. Such systems can allow to set the desired time-averaging window (
Discussion
In this study, the implications of the RF EMF limits specified in
Within some meters from the BS, the effect of the environment on the incident power density is small and the BS compliance boundaries derived in free space are deemed to be accurate (
The results presented in Section 4.3 for frequencies above 6 GHz are derived from the reference levels. Consolidated measurements and numerical methods addressing the basic restrictions above 6 GHz, i.e., absorbed power density, for the purpose of evaluating EMF compliance, are in fact not yet available. Few initial studies, e.g. (
According to
FIGURE 12

Reactive near-field boundaries for the BSs antennas selected in Section 4.
Conclusion
In this work, an analysis of the implications that the recently updated RF EMF exposure guidelines by ICNIRP have on EMF compliance of BSs has been conducted. A few changes are introduced by
For macro BS, the compliance boundary dimensions applicable for the general public remain substantially unchanged, if assessed using
For indoor low-power BS, the low EIRP leads to exclusion zones which extend only up to a few centimeters. For these, no difference in the compliance distance between
Standardization committees, such as IEC TC106, have developed exposure assessment methodologies for mMIMO BS by considering that antenna patterns are changing rapidly during operation, and beams are formed to optimize the transmission towards the served devices. Due to beam-steering, the maximum time-averaged power per beam is lower than the instantaneous rated maximum and the ratio between these two is often referred to as power reduction factor (PRF). Previously established PRFs based on 6-min time averaging (or over shorter times at higher frequencies, e.g., about 2 min at 30 GHz), are conservative with respect to the 30 min whole-body averaging interval specified within
Exposure assessments of BS are typically conducted outside the reactive near-field region of the antenna, where incident power density or field strength limits (i.e., the reference levels) apply. The only exception might be for very low power BS operating below 6 GHz, for which compliance is typically assessed based on SAR. Therefore, the restrictions introduced by
Statements
Data availability statement
The original contributions presented in the study are included in the article/Supplementary Materials, further inquiries can be directed to the corresponding author.
Author contributions
Conceptualization, all.; methodology, DC and BX; formal analysis, DC, BX, DS and CT; writing-original draft preparation, DC; writing-review and editing, all. All authors have read and agreed to the published version of the manuscript.
Conflict of interest
Authors DC, BX, DAS, PJ, FG, CD and CT are employed by company Ericsson AB.
Publisher’s note
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.
Supplementary material
The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/frcmn.2022.744528/full#supplementary-material
Footnotes
1.^The whole-body exclusion criteria discussed in Section 4.2 are also valid below 6 GHz (as the whole-body SAR, limit given by
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Summary
Keywords
5G, base stations, mobile technologies, ICNIRP, RF EMF compliance
Citation
Colombi D, Xu B, Anguiano Sanjurjo D, Joshi P, Ghasemifard F, Di Paola C and Törnevik C (2022) Implications of ICNIRP 2020 Exposure Guidelines on the RF EMF Compliance Boundary of Base Stations. Front. Comms. Net 3:744528. doi: 10.3389/frcmn.2022.744528
Received
20 July 2021
Accepted
06 January 2022
Published
04 March 2022
Volume
3 - 2022
Edited by
Rosdiadee Nordin, Universiti Kebangsaan Malaysia, Malaysia
Reviewed by
Chee Yen (Bruce) Leow, University of Technology Malaysia, Malaysia
Chiara Lodovisi, Consorzio Nazionale Interuniversitario Per Le Telecomunicazioni, Italy
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Copyright
© 2022 Colombi, Xu, Anguiano Sanjurjo, Joshi, Ghasemifard, Di Paola and Törnevik.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Davide Colombi, davide.colombi@ericsson.com
This article was submitted to Wireless Communications, a section of the journal Frontiers in Communications and Networks
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