Radiation Protection Dosimetry (2004), Vol. 111, No. 4, pp. 339–342 doi:10.1093/rpd/nch050 RAY-TRACING TECHNIQUES TO ASSESS THE ELECTROMAGNETIC FIELD RADIATED BY RADIO BASE STATIONS: APPLICATION AND EXPERIMENTAL VALIDATION IN AN URBAN ENVIRONMENT S. Adda, L. Anglesio1, G. d’Amore1, M. Mantovan1 and M. Menegolli2 1 ARPA Piemonte, Dipartimento di Ivrea, Via Jervis 30, 10015 Ivrea (To), Italy 2 Provincia di Torino, Area Ambiente, Via Valeggio 5, 10128 Torino, Italy INTRODUCTION A careful assessment of the exposure of urban populations to electromagnetic fields, generated by radio base stations for mobile telephones, requires the use of deterministic models that take into account the interferences caused by the buildings in the propagation of the field. One of these models is based on the ray-tracing method, which allows the simulation of the propagation of electromagnetic waves between the transmitting antenna and the reception point by taking into account the influence of all reflection and diffraction phenomena due to the presence of obstacles in the propagation area, on the basis of the theory of geometrical optics and other related developments [Geometrical Theory of Diffraction (GTD)/Uniform Theory of Diffraction (UTD)]. Although it is possible to model very complex urban environments using such a method, it is often impossible to get all the input data needed to take into account, for instance, the geometrical and electrical features of the buildings within a certain urban area. Moreover, the knowledge of such features always suffers from uncertainties that influence the accuracy of the calculated results. The aim of this paper is to estimate the uncertainties in the application of the ray-tracing method in different urban environments through several measurements planned in order to experimentally validate the adopted code (the VIGILA 3.0 software). This is necessary because of the lack of comparisons in the literature between calculations with ray-tracing techniques and measurements of significant environment field levels, carried out in Corresponding author: s.adda@arpa.piemonte.it order to assess the exposure of the population and compare it to the legal limits. Such a validation has been carried out through narrow band measurements in both near- and far-field situations. MATERIALS AND METHODS Ray-tracing techniques and the adopted model Ray-tracing techniques allow the estimation of the propagation of electromagnetic waves in complex environments by taking into account the presence of obstacles and on the basis of the laws of modern geometrical optics. The interference caused by the obstacles is estimated by first calculating the transmission and reflection coefficients, which depend on the angle of incidence of the rays and on the electrical features of the materials [Luneberg–Kline’s theory concerning asymptotic developments(1,2)]. Similarly, GTD and UTD require the evaluation of diffraction coefficients, which also allow a ‘geometrical’ treatment of this phenomenon. Ray-tracing methods can be used at high frequencies, namely when the obstacle dimensions are large in comparison with the wavelength, and therefore it is correct to describe electromagnetic wave propagation by means of optical rays. In order to assess the propagation path, and calculate the electric field along each path, it is necessary to model the ground and buildings by taking into account the geometrical and electrical descriptions of the propagation environment. The tested software (VIGILA 3.0), which was developed by TiLab laboratories, implements a backward ray-tracing technique, taking into account the first- and second-order contributions, for six 339 Radiation Protection Dosimetry Vol. 111, No. 4 ª Oxford University Press 2004; all rights reserved Downloaded from http://rpd.oxfordjournals.org/ at Freie Universitaet Berlin on June 25, 2015 This paper aims to validate a ray-tracing model for electromagnetic field calculation, which is used in urban environments to predict irradiation from radio base stations for population exposure evaluation. Validation was carried out through a measurement campaign by choosing measurement points in order to test different propagation environments and analysing broadcast control channels through narrow band measurements. Comparison of the calculated and measured fields indicates that the ray-tracing model used calculates electric field with good accuracy, in spite of the fact that the propagation environment is not described in detail, because of difficulties in modelling the geometrical and electrical characteristics of urban areas. Differences between the calculated and measured results remain below 1.5 dB, with a mean value of 1 dB. S. ADDA ET AL. possible configurations (direct path, single reflection, double reflection, single diffraction, diffraction– reflection and reflection–diffraction). The software uses a vector database containing three-dimensional cartographic information as well as the building material used for each building as input. Based on these data, the software calculates the visibility array and the possible optical paths between the source and the reception points. Experimental validation (1) a receiving biconical antenna (Australian Research PBA10200) with frequency response in the 100 MHz–2.1 GHz range; (2) a Rohde & Schwarz FSP-3 spectrum analyser, with frequency response in the 9 kHz–3 GHz range; (3) a Suhner 20 m coaxial cable. For both types of areas examined, the evaluation of the fields was carried out using the VIGILA software and by creating the appropriate geometrical and electrical models for the urban area, in order to characterise the propagation environment. Cartographic information for Site 1 (Figure 2a); on a 1 : 1000 scale was extracted from a database for the urban area of the city of Turin, whereas for Site 2 the reconstruction of the propagation environment required a greater accuracy because the measurements were carried out in near-field conditions (Figure 2b). For this purpose, a building planimetry on a 1 : 50 scale was used, digitizing every structure (dividing walls, brick chimneys, etc.) using an AUTOCAD application. In order to evaluate reflection and transmission coefficients for each building, the prevailing type of building material was assessed by inspection and the corresponding dielectric constants were chosen from among the list of standard walls supplied by the VIGILA software. The buildings were placed on a DTM obtained by interpolation using the spline method(4) and the topographical points of the cartographic information (on a scale of 1 : 1000) of the city of Turin. RESULTS Figure 1. Sampling grid. The ray-tracing model was used to compare the measured and calculated electric field levels by taking an average for the 12 points on the grid. The four sites considered are different with respect to the propagation conditions: Site 1A is an uncovered car park located on the third floor with the 340 Downloaded from http://rpd.oxfordjournals.org/ at Freie Universitaet Berlin on June 25, 2015 The ray-tracing model was validated through several measurements that were carried out in certain areas of the city of Turin. These areas were chosen according to the following criteria: the availability of particularly detailed and up-to-date vector cartography, the type of urban environment and the presence of significant electric field levels with respect to the urban background(3). To select the areas with higher field levels, the distribution of the electromagnetic field generated by radio base stations was assessed, for the entire municipal territory, by means of a simplified far-field calculation model. The field was calculated at a height of 1.5 m from the ground, using the digital terrain model (DTM) on a grid of points with a 50 m step. The data obtained allowed the determination of areas with theoretical levels of electric fields between 1.5 and 3 V/m, often characterised by the presence of several radio base stations coexisting at the same site. Two types of sites were thus selected: the first site (referred to as Site 1) was located in a far-field zone, where measurements were carried out at locations with different visibility situations; the second site (referred to as Site 2) was a terrace, where three radio base stations were set up and where measurements were carried out under near-field conditions. For each measurement site, electric field sampling was carried out at points located at the corners of a 1 m box, at three different heights from the ground level for 12 points overall (Figure 1). Then the average of the field levels measured at the 12 grid points was calculated in order to compare the calculated and measured values. For each radio base station, a narrow band measurement at each grid point was carried out, detecting only the control channel, which is always active at constant power (the Broadcast Control Channel of Global System for Mobile communication). The assessment of the electric field level by control channel detection made the measurement independent of the working conditions of the radio base station. The instrumental apparatus, which includes an electrically insulated van to ensure electromagnetic immunity, comprises the following parts: EXPERIMENTAL VALIDATION OF RAY-TRACING TECHNIQUES (a) (b) Table 1. Comparison between the average values of the measured and calculated electric field levels obtained using the ray-tracing technique at the different sites. Measurement Emeas (V/m) site Site Site Site Site 1A 1B 1C 2 0.810 0.025 0.100 1.623 0.158 0.005 0.021 0.358 Ecalc (V/m) SEcalc (%) 0.952 0.023 0.127 1.895 0.032 0.001 0.006 0.022 17.5 8.0 27.0 16.8 obstacles between the source and the evaluation point and the field values are very low, the calculated level is slightly lower than the measured level. The same data reported in Figure 3 show a good agreement between the calculated and measured values as the difference between these values is, for each site, within the uncertainty of the measured level. CONCLUSIONS radio base station within its line of sight, Site 1B is a green area located at about 300 m from the radio base station installation site with several buildings in between, Site 1C is a green area under shadow conditions due to one single row of buildings between the source and the measurement point and Site 2 is the building terrace where the radio base stations are located (the calculation is made by using the near-field algorithm supplied by the VIGILA software). The results for the different measurement sites are indicated in Table 1, which lists the measured electric field levels and the field levels calculated using the model. The uncertainty associated with each measured value was obtained by adding the instrumental uncertainty and the standard deviation of the distribution of the values measured on the considered volume, which is related to the uncertainty due to antenna positioning. The standard deviation of the calculated values [s/H(n 1)], in the volume considered for each measurement site, was assessed to estimate the uncertainty for the average calculated field level (SEcalc). The last column in Table 1 lists the percentage difference () between the calculated and measured levels. It is noticeable that the measured and calculated data differ by 8–27%. In three of the four sites the calculated level is higher than the measured level; only in the case of Site 1B, where there are several This research shows that there is a good agreement between the results of ray-tracing calculations and the measurements made in urban environments under different propagation conditions. It is highly significant that the differences between the calculated and measured data are always within the measurement uncertainty even if approximations such as morphologic data of the urban propagation area, topographical data of the transmitting antennae and characterisation of the surfaces (considered perfectly flat and smooth), and the temperature and humidity conditions when carrying out the measurements were not taken into account in the uncertainty estimation. In particular we emphasise the agreement obtained in those sites where there are buildings in between (Sites 1B and 1C) and where a simple calculation under free-space and far-field conditions led to an overestimate of the field by 2–12 times the measured value. It has to be pointed out that under visibility conditions also the results of the ray-tracing model come closer to the measured levels compared with the simulations under far-field conditions: in Site 1A the far-field model gives an overestimate of 59% compared with the measured level, whereas in Site 2 we find an overestimate of 30% (in both cases the overestimate is higher than the uncertainty in the experimental value). This validation demonstrates that a ray-tracing model is an useful instrument for population 341 Downloaded from http://rpd.oxfordjournals.org/ at Freie Universitaet Berlin on June 25, 2015 Figure 2. Three-dimensional model of the measurements and calculation sites. Electric field (V/m) S. ADDA ET AL. 2 1.5 Emeas E ray-tracing 1 E far field 0.5 0 SITE1A SITE1B SITE1C SITE2 Figure 3. Comparison between the measured and calculated electric field levels obtained using the ray-tracing model at the different sites. 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