2. Materials and Methods
To determine workers’ exposure to private 5G networks, a large number of measurements were conducted in combination with numerical calculations to precisely determine the compliance zones. Several exposure scenarios were measured and numerically modeled, including production facilities, logistics, offices and research facilities with different types of installations: private standalone (SA) and non-standalone (NSA) 5G networks at 3.5 GHz and 26 GHz, as well as public 5G networks with private slicing (
Table 1).
First, all necessary technical data about the RF EMF sources were obtained, such as operating frequency, transmission power, and antenna characteristics. Such information is required for numerical modeling and the proper design of the measurement procedures (
Figure 1).
Measurements were performed according to the widely applied IEC 62232:2022 standard [
3]. To assess the worst-case exposure, measurements under load and selective measurements were used [
3]. Measurements under load are possible when the measured source is predominant, as the traffic is generated mainly by the measured source. For selective measurements, the amplitude of the Secondary Synchronization Signal (SSS) with constant power is measured with a code-selective instrument equipped with a 5G decoder. According to IEC 62232:2022 [
3], the extrapolation to the maximum
E-field is calculated according to the formula:
where
Emax is the maximum value of
E field for an individual 5G BS cell,
nRE,SSS is the ratio between the maximum permitted transmission power and resource element (RE) power,
FTDC is the Time Division Duplex (TDD) duty cycle,
Fant is the beamforming factor due to different antenna gains of the transmitting SSS and the physical downlink shared channel (PDSCH) (1 if no beamforming),
BF is the boosting factor for the reference signal (RS), and
ERE,SSS is the measured RE power in SSS.
nRE,SSS is determined by the signal bandwidth and subcarrier spacing (SCS) and is given in the standard IEC 62232:2022 [
3]. The beamforming factor
Fant is calculated from the radiation pattern of the antenna according to the equation:
where
GPDSCH (in dBi) is the antenna gain when transmitting the PDSCH signal,
AtPDSCH (in dB) is the envelope of relative attenuation of the antenna when transmitting the PDSCH signal in the direction of evaluation in dBi, and
GSSS (in dBi) is the antenna gain when transmitting the SSS and
AtSSS (in dB) is the envelope of relative attenuation of the antenna when transmitting the SSS in the direction of evaluation. For selective measurements of 5G, several technical parameters are required, compared to only minimal technical data necessary for measurements under load.
All measurements were performed with a spectrum analyzer (Narda SRM-3006) combined with a Narda 3502 three-axis antenna for FR1 and a Narda LNB 1 horn antenna for FR2 (all three Narda STS, Pfullingen, Germany). The expanded measurement uncertainty of the equipment was ±3.5 dB for the FR1 frequency band and ±3.1 dB for the FR2 frequency band.
Part of the measurements were carried out at different distances from the antenna in the direction of the main beam, 45° to the left or right of the main beam, 90° to the left or right of the main beam, and below the antenna, depending on the antenna installation. The results of these measurements were used to confirm the numerically calculated compliance distances. Part of the measurements were conducted on a uniform grid across the entire targeted area to capture the distribution of the exposure. The measurement height was 1.5 m above the ground, serving to estimate typical exposures. For all measurement locations, the vertical and horizontal distances from the antenna were determined.
To assess time variability, time-controlled measurements were performed at one representative location for most scenarios, spanning from a few minutes to more than 1 h. This enabled the calculation of various averaging periods and the estimation of ratios between typical and maximum exposures.
For each antenna considered in the simulations, the compliance boundaries (CD) were determined by evaluating the compliance distance in all directions around the antenna. CD is the minimum distance from the antenna at which the power density no longer exceeds the reference level limit
Slim. CD was derived using the spherical far-field formula for power density [
3]:
where
S is the radiated power density (W/m
2),
P is the input power to the antenna (W),
G(
θ,
φ) is the linear gain of the antenna,
r is the radial distance from the antenna (m),
θ is the polar (elevation) angle, and
φ is the azimuthal angle.
Setting
S =
Slim and solving the above equation for
r, we can determine the CD:
This equation provides the direction-dependent compliance distance CD(θ, φ), which varies according to the antenna’s radiation pattern, and is applied under the assumption of free-space propagation, i.e., that no significant reflecting surfaces or objects are present in the direction of evaluation. Using this formulation, we computed the 3D iso-surface compliance boundary, which defines the smallest closed surface surrounding the antenna where the power density equals Slim in all directions. Additionally, we derived the box-shaped compliance boundary, defined as the smallest axis-aligned bounding box that entirely encloses the 3D iso-surface. This box provides a simplified geometric representation useful for compliance zoning. CDs were determined for the worst-case exposure situation when the antenna operated at maximum power.
In
Figure 2, an example of compliance boundaries for the Alpha Wireless AW3232 Base Station sector antenna is given. It assumes a transmitted power of 4 W. At the top, a 3D iso-surface is given representing the CD. At the bottom, vertical plane (left) and horizontal plane (right) cross-sections are shown. For the vertical plane, the maximum CD was obtained at a polar angle φ of −43° and for the horizontal plane at an elevation angle θ of 93°. The blue line shows the CD, whereas the red line represents the box-shaped CD.
A MATLAB (version R2025a) program package (MathWorks, Natick, MA, USA) was used for the numerical determination of the CD.
4. Discussion
RF EMF measurements were conducted across eight distinct scenarios, selected to represent a diverse range of sectors—including logistics, manufacturing, and office environments—and frequency bands (3.5 GHz, 26 GHz). The selected scenarios encompass a broad spectrum of private network settings, ranging from public 5G macro slices operating at 100 W per sector to indoor pico cells with power below 1 W.
However, the selection process was significantly constrained by several external challenges. First, the number of fully operational private 5G installations remains very limited. Second, the owners of the existing private 5G networks were generally reluctant to grant access to their facilities, which hindered the execution of more extensive measurement campaigns.
Another significant challenge was the current lack of network traffic. Most private 5G networks are currently idle or carry minimal traffic, particularly regarding the number of active connected devices. Although 5G for Industry 4.0 is envisioned to facilitate massive connectivity for IIoT devices and user interfaces, only a few devices were active during these measurements. The CD values presented in
Table 2 and the typical exposure levels in
Table 15 were determined for worst-case conditions; consequently, they remain independent of actual network traffic or device use. However, in environments with a high density of connected devices, the overall exposure to RF EMF may increase—particularly if there is substantial uplink traffic, which is a possible future scenario for private networks. Due to the limited number of such devices in this study, it was not possible to analyze these cumulative effects. Notably, the literature regarding general public exposure indicates that the simultaneous operation of a large number of devices in dense situations can lead to a marginal increase in total RF-EMF exposure [
6,
7].
Nevertheless, time-variability measurements were conducted across key scenarios, where the total value was measured across the frequency band in which the network was operating. Where traffic was present—or deliberately generated—information regarding time variability and average exposure was obtained. However, estimating expected average exposure values in private 5G networks remains challenging, constrained by their current limited operational state. To address this, worst-case conditions were determined in all scenarios, either by selective measurements with extrapolation to maximum values or by performing measurements under forced traffic conditions (e.g., speed tests or continuous data transfer).
During the measurement process in an operational factory environment, a location was identified where the pRRH was installed at a lower height of 3.1 m, representing the worst-case exposure scenario. At this location, the maximum electric field measured at a height of 1.5 m was 3.1 V/m, recorded right below the pRRH.
Table 15 summarizes the raster measurement results. Raster measurements were selected because they provide the best estimate of the RF EMF levels emitted by the equipment under test. By distributing measurement points throughout the entire area surrounding the source, they yield a reliable assessment of the average RF EMF exposure for personnel in the vicinity of the private wireless network.
The results presented in
Table 15 demonstrate significant variability across the different exposure scenarios, with values spanning a factor of up to 20. Notable spatial variability is also evident within individual scenarios. For scenarios 2, 3, 4, 5, and 8, the ratio between the median and maximum values is below 4, indicating relatively uniform exposure levels across the measurement grid. In contrast, this ratio exceeds 10 in scenario 1. This marked discrepancy is attributed to the antenna’s low installation height (1.9 m), which placed the closest measurement point directly in the main beam and at a short distance from the antenna.
Determination of CD through both calculations and measurements indicates that, for typical private 5G installations, compliance zones are relatively compact: below 1.5 m for general public exposure and below 0.7 m for occupational exposure. An exception occurs when a network slice within a public 5G network is utilized as a private network; in these instances, compliance zones increase to below 15 m for general public exposure and below 6 m for occupational exposure. It should be noted that these calculated CDs represent conservative, worst-case situations, as the source was modeled as a single-point source. If the source were instead modeled as an array of emitters—more accurately reflecting the construction of a real antenna—the resulting compliance zones would be smaller. These findings are supported by the experimental data: in cases where measurements were conducted close to the source, the CDs derived from measurements were consistently smaller than those derived from numerical calculations.
Regarding time variability, the investigation demonstrated that the averaging duration has a limited impact on selective measurements. In the four scenarios analyzed, the maximum difference between the 1 min and 6 min averages was 33%, and below 10% when comparing the 3 min average.
In contrast, measurements across the entire 5G frequency band exhibited substantially greater variability, driven primarily by the network’s operational state. Although the base stations were active, they carried traffic only for a small fraction of the time; consequently, intermittent bursts of high traffic significantly influenced the calculated average. The maximum difference between 1 min and 6 min averages reached 100%. Furthermore, pronounced differences were observed when comparing periods of high-demand speed testing against baseline idle periods.
In scenario 5: Office, test facility of wireless networks, private 5G FR1 micro cell, the only active device was the modem used for speed testing, which encompassed both download and upload phases. Measurements during these active periods differed markedly from those obtained during idle times. A similar trend was observed in scenario 1: Logistic sector: port, private 5G FR1 micro cell: during periods of low traffic, the electric field remained slightly above 1 V/m, whereas it increased 2.5–5 V/m during active traffic conditions.
Spatial variability was assessed across several exposure scenarios using the methodology prescribed by IEC 62232:2022 [
3]. The spatial averaging scheme utilized three vertical heights (1.1 m, 1.5 m, 1.7 m) and three lateral positions (center, 0.2 m left, 0.2 m right), yielding nine measurements. Two additional vertical planes (0.2 m in front and 0.2 m behind) increased the total to 27 measurement points.
In scenario 2: Logistic sector: port, public slice 5G FR1 macro cell, the source consisted of a 5G network slice utilizing a beamforming macro cell mounted on a pole. All pilot signal results were consistent across all averaging schemes: individual measurements ranged from 0.095 to 0.228 V/m, with calculated averages ranging from 0.136 to 0.151 V/m. However, the extrapolated maximum values exhibited greater variability due to beamforming effects. Despite the close spatial clustering of measurement points, the extrapolation factor varied between 215.28 and 270.56. Consequently, extrapolated values ranged from 20.80 to 48.99 V/m, whereas the averaged values were more stable, ranging from 32.27 to 36.42 V/m. Notably, the differences between the various averaging methods remained insignificant. Similar trends were obtained for scenario 5: Office, test facility of wireless networks, private 5G FR1 micro cell, where the values ranged from 9.35 V/m (single point) to 12.71 V/m (three-point average).
In contrast, scenario 7: Research facility, private 5G FR2 micro cell, demonstrated significant variation between averaging methods, heavily influenced by measurement height. This result was expected given the short distance between the measurement location and the highly directive base station antenna. Minor changes in antenna height caused substantial fluctuations in antenna gain and, consequently, in the measured electric field strength. The disparity in the data is notable: the maximum single-point value reached 48.55 V/m, while the nine-point average at 1.1 m yielded a minimum of 12.16 V/m. The sensitivity to height is further evidenced by comparing the nine-point averages: the value was 47.50 V/m at 1.5 m, but dropped sharply to 14.73 V/m at 1.7 m.
Spatial variability measurements indicate that when antennas possess low directivity and are measured at a sufficient distance, the precise micro-location of the measurement point usually has no significant influence. Conversely, for highly directional antennas, the micro-location of the antenna has an important effect on the measured value.
Time and spatial variability are also substantially affected by the beamforming technology. While the effects of beamforming were not explicitly analyzed in this study, the methodologies for determining CD were designed to be conservative: for calculations, the envelope of all traffic beams was utilized, whereas for measurements, maximum values were determined without applying power reduction factors.
Although the effects of beamforming have been extensively analyzed for public networks [
8,
9], the current lack of representative traffic and real-world usage in the analyzed private networks precluded an analysis of the beamforming’s influence on actual exposure levels.