Basic standard for the calculation and measurement of electromagnetic field strength and SAR related to human exposure from radio base stations and fixed terminal stations for wireless telecommunication systems (110 MHz - 40 GHz)

This basic standard applies to radio base stations and fixed terminal stations for wireless telecommunication systems as defined in Clause 4, operating in the frequency range 110 MHz to 40 GHz. The objective of the standard is to specify, for such equipment, the method for assessment of compliance distances according to the basic restrictions (directly or indirectly via compliance with reference levels) related to human exposure to radio frequency electromagnetic fields.

Grundnorm für die Berechnung und Messung der elektromagnetischen Feldstärke und SAR in Bezug auf die Sicherheit von Personen in elektromagnetischen Feldern von Mobilfunk-Basisstationen und stationären Teilnehmergeräten von schnurlosen Telekommunikationsanlagen (110 MHz bis 40 GHz)

Norme de base pour le calcul et la mesure des champs électromagnétiques et SAR associés à l'exposition des personnes provenant des stations de base radio et des stations terminales fixes pour les systèmes de radiotélécommunications (110 MHz - 40 GHz)

Osnovni standard za izračunavanje in merjenje moči elektromagnetnega polja in SAR v povezavi z izpostavljenostjo ljudi sevanjem zaradi radijskih baznih postaj in fiksnih terminalskih postaj za brezžične telekomunikacijske sisteme (110 MHz - 40 GHz)

Ta osnovni standard velja za radijske bazne postaje in fiksne terminalske postaje za brezžične telekomunikacijske sisteme, kot je določeno v Klavzuli 4, ki delujejo v frekvenčnem razponu od 100 MHz do 40 GHz. Namen tega standarda je za takšno opremo določiti metodo za ocenjevanje dogovorjene razdalje v skladu z osnovnimi omejitvami (neposredno ali posredno s skladnostjo z referenčnimi stopnjami), povezanimi s človeško izpostavljenostjo elektromagnetnim poljem radijske frekvence.

General Information

Status
Withdrawn
Publication Date
20-Jun-2013
Current Stage
9960 - Withdrawal effective - Withdrawal
Start Date
27-Sep-2020
Completion Date
27-Sep-2020

Relations

Buy Standard

Corrigendum
EN 50383:2010/AC:2013
English language
22 pages
sale 10% off
Preview
sale 10% off
Preview
e-Library read for
1 day

Standards Content (Sample)


2003-01.Slovenski inštitut za standardizacijo. Razmnoževanje celote ali delov tega standarda ni dovoljeno.*+]Grundnorm für die Berechnung und Messung der elektromagnetischen Feldstärke und SAR in Bezug auf die Sicherheit von Personen in elektromagnetischen Feldern von Mobilfunk-Basisstationen und stationären Teilnehmergeräten von schnurlosen Telekommunikationsanlagen (110 MHz bis 40 GHz)Norme de base pour le calcul et la mesure des champs électromagnétiques et SAR associés à l'exposition des personnes provenant des stations de base radio et des stations terminales fixes pour les systèmes de radiotélécommunications (110 MHz - 40 GHz)Basic standard for the calculation and measurement of electromagnetic field strength and SAR related to human exposure from radio base stations and fixed terminal stations for wireless telecommunication systems (110 MHz - 40 GHz)33.070.01Mobilni servisi na splošnoMobile services in general17.220.20Measurement of electrical and magnetic quantitiesICS:Ta slovenski standard je istoveten z:EN 50383:2010/AC:2013SIST EN 50383:2010/AC:2013en01-september-2013SIST EN 50383:2010/AC:2013SLOVENSKI
STANDARD
Corrigendum to EN 50383:2010 English version ___________ Due to a mistake in the numbering, the whole Clause 6 needs to be renumbered. Please note that the content of Clause 6 has not been modified. Replace the entire Clause 6 by the following: 6 Electromagnetic field measurement 6.1 Introduction This section describes the measurement procedures that may be used to assess, at points of investigation, the electromagnetic field components (E and H and therefore the power density) radiated by antennas. The field measurements can be obtained either by surface or volume scanning.
The methods used are to measure directly or indirectly the E-field or H-field strength, deduce the field distribution for a given input power and frequency. 6.2 Surface scanning method 6.2.1 Introduction
Methods to perform surface scanning could be, but are not limited to, far-field, compact range, and planar, cylindrical or spherical near-field as long as the methodology is accurately defined and the uncertainty criteria (Annexes B and E) are fulfilled.
6.2.2 Spherical scanning method Measurements of electric field amplitude, phase and polarisation are made at sufficient points on the surface of a sphere surrounding the EUT to establish the parameters to model a set of isotropic sources on that surface that will produce at the point of investigation the same field as the EUT. To make this valid, the scanned spherical surface shall contain all the relevant energy that is radiated from the EUT. The parameters of this set of isotropic-radiators are then used to calculate the field at the points of investigation required in order to establish the compliance boundary.
The principle steps are summarised in Figure 1. SIST EN 50383:2010/AC:2013

Start Return field value at point of investigation Chart 5.1
Establish characteristics of equivalent isotropic-radiators on surface of radius Rmes and determine E/H at point of investigation scaled for appropriate EUT power level(s) (6.2.4) Review uncertainty (6.2.5) Determine scanning radius & spherical sampling angles, set up test equipment (6.2.2) Measure phase & amplitude and polarization of EUT signals over a spherical surface of radius Rmes. (6.2.3)
Figure 1 – Outline of the surface scanning methodology 6.2.2.1 Measurement equipment 6.2.2.1.1 General description The surface scanning consists of an Equipment Under Test (EUT) mounted on an azimuthal positioner and the probe(s) mounted on a support structure at distance Rmes from the EUT. This method requires the ability to measure the phase of the signal. Detection shall consist of either one probe moved mechanically along the structure or one probe array switched electronically in order to perform an angular elevation scan of the electromagnetic fields.
Alternatively, the EUT can be moved to different elevation angles by means of an additional elevation positioner. The near-field antenna measurement system shall be configured according to Figure 2. SIST EN 50383:2010/AC:2013

Probe
positioning system Vector - receiver Positioner
control synthesizer Data acquisition
and PC
control Probe EUT Y Z X Amplifier (0, 0, 0) Rmes
Figure 2 – Block diagram of the near-field antenna measurement system
The following equipment is required:
- anechoic chamber; - electric probe(s) (antenna(s)); - support structure for probe(s); - supporting structure; - vector receiver; - synthesiser and amplifier(s); - probe positioning system or probe array controller system; - EUT positioning system.
A computer controls the measurement equipment located in the anechoic chamber. The computer shall be placed so as not to influence the measurements.
The test shall be performed using probe antennas providing electric field measurements. The probe antennas shall be accurately positioned to measure the electric field distributions in a spherical surface around the EUT.
The measurement shall be carried out with a minimum of reflections from the environment in order to simulate free space conditions. 6.2.2.1.2 Scanning equipment: positioning and orientation requirements
6.2.2.1.2.1 General criteria The measurement system shall be able to scan a specified spherical surface of the test environment. In order to provide sufficient data required combined with the resolution and accuracy needed for post-processing; − the radius Rmes between the reference point of the EUT (0, 0, 0) and the probe(s) at each of the measurement points shall be chosen to satisfy the radius criteria (ref. 6.2.2.1.2.2) and shall be established within
degrees [see reference Clause B.3].
The sampling of the whole spherical surface is achieved through the rotation of the EUT or the structure supporting the probe(s). Several types of positioning systems are proposed in Annex B. 6.2.2.1.2.2 Radius criteria Rmes the distance between the reference point of the EUT at origin of rotation and the measurement probe(s) shall be the greater of
− Rmin in order to minimise the impact of the non-radiating near fields where Rmin depends upon the maximum dimension of the EUT and Figure 3; and − the distance required to ensure that the probes and measurement equipment is operating within their calibrated level range for the power specifications of the EUT.
-===0° Rmin
-===90° a Reference point of the EUT
-===0° a Rmin
-===90° Reference point of the EUT
WheRmin
Rmin
Where:
a = the minimum radius of a sphere, centred at reference point, that will encompass the EUT. Figure 3 – Minimum radius constraint 6.2.2.1.2.3 Sampling criterion The sampling criterion (also commonly called Nyquist criteria) requires a maximum angular spacing of the measurement points of λ/2 over the sphere circumscribing the EUT with radius Rmes. The angles δφ (azimuth) and δθ (elevation) between adjacent measurements depend on the system but shall comply with the constraints of Figure 4.
Figure 4 – Maximum angular sampling spacing constraint 6.2.2.1.2.4 Constraints on EUT dimensions for specific measurement system
Given the radius Rmes equal to the constant distance between the center of rotation of the EUT and the probe(s), and given the number N equidistant sampling points in elevation or azimuth, each of the above criteria leads to a maximum dimension Dmax for the EUT:
)12(2)(2maxmax−<−<πλλNDandRDmes Where
aD2max=(see Figure 3) Depending on the operating frequency, the maximum size will be limited by the most constraining of both criteria (i.e. the first criteria at lower frequencies and the second criteria at higher frequencies). 6.2.2.1.3 Measurement probe The probe or probe array shall be designed and dimensioned such as not to disturb the electromagnetic fields generated by the EUT. The probe(s) gain shall be calibrated with a measurement uncertainty less than ± 0,5 dB. The probe shall be able to provide orthogonal polarisation with cross-polar isolation better than 30 dB. Alternatively, a second scan with a probe rotated by 90 degrees could detect the cross-polar values. Typically open-ended waveguides (OEW) or crossed dipoles are used, as they have a well-defined radiation characteristic and a low influence on the EUT. 6.2.2.1.4 Supporting structure The antenna shall be mounted on a dielectric holder fixed on the positioning system. The holder shall be made of low conductivity and low relative permittivity material(s): tan(δ) ≤ 0,05 and εr ≤ 5. Alternatively, the antenna may be mounted on a metallic pipe mast, if this is the normal operating situation of the antenna. If the mounting situation differs from a free-space equivalent, this has to be documented in the measurement results. The antenna shall be mounted so that the reference point (0, 0, 0) is in the centre of the sphere.
If no PLL-system is used, the shielding level of the anechoic chamber enclosure should be better than
50 dB at the measurement frequencies. The size and cover materials of the anechoic chamber shall be evaluated in order to minimise the level of perturbation due to reflections. The methodology to evaluate the chamber reflectivity is given in Clause B.3. Ambient temperature shall be in the range of 10 °C to 30 °C and shall not vary by more than ± 5 °C during the test. 6.2.2.3 Measurement protocol 6.2.2.3.1 Calibration of the test facility Four calibrations of the near field spherical test facility shall be performed: - polarisation calibration; - amplitude and phase calibration (uniformity between probe(s)); - gain calibration; - electrical noise evaluation.
The measurement equipment shall be calibrated as a complete system at the appropriate frequencies according to the methodology defined in Annex B. Calibration guidelines are given in Clause B.6. 6.2.2.3.2 Test to be performed The test shall be performed at the fixed power matched to the detection range of the measurement equipment.
Post-processing will derive the results at the desired input power values. For multi-mode and multi-band EUTs, all the previous tests shall be performed in each operating transmitting band (see 5.2). 6.2.2.3.3 General requirements for the Equipment Under Test (EUT) Surface scanning shall be used to define the EUT electromagnetic field parameters. The EUT shall be fed with frequencies comparable to normal configurations. A generator may replace the transmitter providing the input power to the EUT. Power scaling is addressed by the post-processing in 6.2.2.4. For a base station with an integrated antenna, special care has to be taken to phase-lock the system. SIST EN 50383:2010/AC:2013

centre frequency; Fmin lower edge frequency; Fmax
upper edge frequency. Check the value of δφ, φmax, δθ, θmin, θmax, Rmes with: δφ azimuthal increment; φmax maximum azimuthal angle value from the reference; δθ elevation increment; θmin lower edge angle of the circular elevation path; θmax upper edge angle of the circular elevation path; Rmes radius of the scan in elevation; Dmax largest dimension of the EUT (= 2a, Figure 3); λ wavelength. Confirm that the total contribution of interferences and reflected signals is less than – 30 dB below the incident signal.
6.2.2.3.4.3 Test procedure - Confirm proper operation of the probe(s), measurement system and instrumentation. - Mount the EUT in the measurement configuration. - Configure the EUT for optimum output power, at the desired frequency and for the desired operating modes. - Position (or configure) the probe(s) at the initial measurement location. - Perform an initial elevation scan at the reference azimuth position and store the data. SIST EN 50383:2010/AC:2013

- Measure and acquire the electromagnetic fields distribution. - The EUT or the probe(s) are moved incrementally in azimuth with ∆φ angle step around a vertical axis that corresponds also to a symmetry axis for the sphere to be scanned. - Repeat the electromagnetic fields measurement until φi = φmax (with φi = φi-1 + δφ, with imin = 1). - After measurements, perform again a final elevation scan at the reference azimuth position and compare the data with the initial elevation scan. Verify that the final values at the maximum levels are within 5 % of the initial values (influence of the drift due to surrounding equipment and environment). - If the drift is greater than 5 %, repeat the measurements.
6.2.2.4 Post-processing 6.2.2.4.1 General The electromagnetic field values shall be obtained by applying a post-processing technique on the set of measured near field data (see Clauses B.4 and B.5). 6.2.2.4.2 Determining electromagnetic field values outside the scanned surface The electromagnetic fields from the EUT shall be modelled by a number of isotropic sources radiating from the scanned surface. At a point of investigation, the vector sum of the fields radiated by
...

Questions, Comments and Discussion

Ask us and Technical Secretary will try to provide an answer. You can facilitate discussion about the standard in here.