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Journal of Microwaves, Optoelectronics and Electromagnetic Applications

On-line version ISSN 2179-1074

J. Microw. Optoelectron. Electromagn. Appl. vol.17 no.4 São Caetano do Sul Oct./Dec. 2018

http://dx.doi.org/10.1590/2179-10742018v17i41548 

Article

Material Characterization and Propagation Analysis of mm-Waves Indoor Networks

A. Fagiani1 

M. Vogel2 

Arismar Cerqueira S. Jr.1 

1National Institute of Telecommunication, Santa Rita do Sapucaí - Brasil, anderson-fagiani@inatel.br and arismar@inatel.br

2Altair Engineering Inc., Hampton - USA, mvogel@altair.com

Abstract

This paper reports detailed propagation analyses of mm-wave indoor networks based numerical simulations of the wireless coverage and measurements of the propagation coefficient at 28 and 38 GHz. Additionally, material characterization of typical buildings materials used in constructions are presented, including: common brick (with and without electrical installations); plaster walls; glazing, Eucatex panels; wooden doors. The computational simulations have been performed using Altair WinProp™ software in order to predict path loss in LOS (Line-of-Sight) and NLOS (Non-Line-of-Sight) environments. The obtained results contributes to the planning of the fifth Generation of mobile communications networks (5G), operating in mm-waves.

Index Terms 5G; indoor propagation; millimeter waves; propagation and wireless communications

I. INTRODUCTION

In recent years, the access networks of telecommunication operators have needed increasing data transfer rates and bandwidth to support all the data traffic generated by their subscribers. The global mobile data traffic is estimated to increase 7-fold between 2016 and 2021, with annual growth rate of 47% [1]. By 2021, it is estimated to reach 48,951 exabytes per month [1]. The International Telecommunication Union (ITU), in one of its reports [2], forecasts in the period from 2020 to 2030 global data traffic will grow from 10 to 100 times. Those forecasts have motivated the search for new frequency bands with enough bandwidth to meet the growing demand for mobile communications, since the traditional UHF and SHF bands are both already congested with the existing services. The millimeter-wave frequency bands (mm-waves) promise to meet this demand. The developing fifth generation of mobile communications networks (5G) intends to use the millimeter-wave frequency bands to obtain the bandwidth required to meet the full demand of carrier subscribers and ensure the deployment success of Gbps per user.

The millimeter-wave frequency bands around 28 and 38GHz have been considered potential for 5G, since they but is significantly increase attenuation due to atmospheric gases absorption [3] and rainfall [4], as shown in Figs. 1 and 2, respectively. In fact, only the attenuation due to the communication channel in mm-waves will be higher, when compared to the attenuation in at microwave frequencies, which are used today for wireless access. However, this can be mitigated by using high-gain adaptive antennas and transmission cells (clusters) with dimensions in the order of 200 m or even less, such as picocells and femtocells [5].

Fig. 1 Signal attenuation due atmospheric gases. 

Fig. 2 Signal attenuation due rainfall. 

This paper first presents material characterization based on measurements of the reflection coefficient and transmission loss of common Brazilian building materials at 28 and 38GHz. Next, it reports a detailed analysis on path loss and propagation coefficients based on experimental measurements and computational simulations performed with Altair WinProp™, using the previously determined reflection and transmission coefficients. LOS (Line-of-Sight) and NLOS (Non-Line-of-Sight) environments have been considered in order to evaluate real scenarios of the future 5G networks. The paper is structured in four sections. Section II describes the methods used in the experimental setup to obtain the reflection coefficient and penetration losses of typical building materials. Section III presents the experimental results of the path loss and propagation coefficient in indoor environments with LOS and NLOS, whereas conclusions and proposals for future works are described in Section IV.

II. Material Characterization

A. Penetration Loss

Penetration loss is the signal attenuation caused by its propagation through a material. It can be defined as the difference between received power in free space [Fig. 3a] and that obtained with an obstructing material between TX and RX, according to Fig. 3b. Equation (1)) calculates the deterministic value of the received power, in which ECL (Excess Channel Loss) is the attenuation added to the communication channel due to the inclusion of the obstructing material between TX and RX [6]:

PR(d)=PT+GT+GR20log(4πd0λ)ECL (1)

Fig. 3 Experimental mounting used in the penetration loss characterization. 

where PT and PR are the transmitting and receiving power in dBm, GT and GR are the gain of transmitting and receiving antennas in dBi, λ is the wavelength (10,71 mm at 28GHz and 7,89 mm at 38GHz). The reference distance d0 was defined as 0,75 m, which is large enough to ensure that characterization analyses occur in the antenna Fraunhofer region (far-field).

The transmitting system was a Keysight signal generator, EXG N5173B model, with operation frequency range from 9 kHz to 40 GHz. The receiving system was a FieldFox Microwave Analyzer, N9952A model, with operation frequency range up to 50 GHz. The generator output power was set to 0 dBm EIRP (effective isotropic radiated power), according to the Table I. The cables and connections characterizations were performed in the PNA Networks analyzer, model N5114A with operation frequency range from 10 MHz to 43.5 GHz.

Table I SETTINGS OF TRANSMITTING SYSTEM 

Parameter Frequency
28 GHz 38 GHz
Antennas horn horn
Gain (TX and RX) 12.6 dBi 13.4 dBi
Losses in cables and connectores 15.84 dB 19.89 dB
Power 3.24 dBm 6.49 dBm
EIRP 0 dBm 0 dBm
Half power angle 19° (V) 16° (V)
20.7 (H) 18.2 (H)
Height of installation from the floor 1.70 m 1.70 m

The analyzed materials were brick walls with and without electrical installations, plaster walls, Eucatex panels, glass (doors and windows) and MDF (Medium Density Fiberboard) doors. Fig. 4 presents the photographs of the material characterization in the free space and some of the investigated materials.

Fig. 4 Experimental mounting used in the penetration loss characterization of brick wall and transparent glass. 

B. Reflection coefficient

The magnitude of the reflection coefficient can be defined as the ratio between the reflected and LOS received powers, according to Equation (2)) [7]. The analyzed surface of the testing material was considered much larger than the distances d1 and d2, as shown in Fig. 5b [6]. Both distances d1 and d2 were in the far field region, with 1.5 and 2.5m for the brick wall and glass characterization, respectively. The parameter dLOS is the free space distance (Fig. 5a).

|Γ|=d1+d2dLOS(PR)refl(PR)LOS (2)

Fig. 5 Experimental setup used in reflection coefficient characterization. 

The reflection coefficient was experimentally obtained for the white brick walls with a thickness of 15.5cm and for 0.8 cm transparent glass. For those experiments, the transmitting power was reduced to −10dBm. In the measurement of the glass reflection coefficient, a horn antenna with the following electromagnetic properties has replaced the transmitting antenna: 24.85dBi gain; 10° half power beamwidth in the magnetic field plane; 9° half power beamwidth in the electric field plane. The motivation for this alteration is increasing EIRP in order to obtain lower standard deviation. The measurements were performed in the vertical polarization at 28 and 38GHz.

Fig. 6 Experimental mountings used in the glass reflection coefficient characterization of brick wall and transparent glass. 

C. Material Characterization

Measurement campaigns were carried in the National Institute of Telecommunications - (Inatel) campus in the city of Santa Rita do Sapucaí in Brazil. The received power in free space was −46.31dBm at 28GHz and – 49.77dBm at 38GHz. In both cases, the TX-RX distance was 0.75m as indicated in Fig. 1a. Table II summarizes the measured penetration loss of the evaluated materials. The ECL parameter represents the average value in dB of the 1,000 measurements for each material. The maximum standard deviation of the measured power was 1.3dB. In addition, Table III summarizes the measured reflection coefficient obtained for brick wall and glass at incidence angles equal to 15°, 45° and 60°.

Table II PENETRATION LOSS MEASUREMENTS 

Material Total Thickness (cm) ECL (dB)
28 GHz 38 GHz
Polarization Polarization
V H V H
Brick Wall with electric installations 15.5 34.93 38.93 48.09 37.52
Brick Wall without electric installations 15.5 30.17 31.63 39.16 33.89
Plastered Walls 11.2 2.73 3.60 2.97 5.56
Eucatex® wall partition panels 3.6 2.45 3.25 4.53 7.31
Slightly dark glass 0.8 3.22 4.10 5.58 6.72
Wooden MDF door 4.0 12.58 16.12 16.74 13.76

Table III REFLECTION COEFFICIENTS 

Material Incident angle (θ) Frequency |Γ|
Brick Wall 15° 28 0.648
38 0.889
45° 28 0.591
38 0.678
60° 28 0.928
38 0.571
Transparent Glass 15° 28 0.502
38 0.894
45° 28 0.843
38 0.522
60° 28 0.591
38 0.447

III. Indoor Environment Characterization

A. Penetration Loss and Propagation Coefficient Estimation

The path loss in a communication channel is defined as the difference between the transmitted and received signal powers [8]. The intensity of the received signal will be a logarithmic distance-decay function, which will express the value of the channel path loss[8]. The angular coefficient of this curve implies in the signal attenuation value, i.e., how much the communication channel will degrade the signal propagation. The angular coefficient is known as the communication channel propagation coefficient.

A propagation coefficient equal to 2 represents free-space condition. Larger propagation coefficients occur when there are obstructions in the propagation channel, causing more channel attenuation. The path loss (PL¯) weighted by the propagation coefficient (n) is a random variable, with distance-dependent log-normal distribution around the mean value, as expressed in Equation (3)). This random variable represents the received signal intensity variations, caused by the path obstructions.

PL¯=PL¯(d0)+10nlog(dd0)+Xσ (3)

Where Χσ is the random variable with a Gaussian distribution with mean of zero and standard deviation of σ in dB [8]. Once the path-loss measurements have been made, the propagation coefficient can be estimated by non-linear regression mathematical algorithms, so that the mean square error between measured and modeled points is minimized according to Equation (4)) [9]. The regression model, as proposed in [10] [11], considers the log-distance propagation model:

n=PR(d0)PR(dRX)10{log(dRXdk)log(d0dk)} (4)

where PR is the measured power at the receptor, d0 and dRX are respectively the reference distance and the distance between TX and RX, dk is the spacing between two successive samples of the measured signal.

B. Experimental results of path loss and reflection coefficient

The same transmission parameters used in the material characterization have been used in the pathloss analysis. An indoor environment of the second floor of Buildings 2, 3 and 4 from Inatel has been considered either in the computational simulations and experiments. Simulation methods in Altair WinProp are mostly based on ray tracing. For indoor simulations, several options exist, with tradeoffsin accuracy and computational time. Fig. 7 illustrates the main options, namely: Multi-Wall Model; Standard Ray Tracing; Dominant Path Model. In the Multi-Wall Model (Fig. 7, left), a ray travels in a straight line from transmitter to receiver. The path loss depends on distance and number of walls the ray passes through. This method is very fast and may be beneficial in large and complicated indoor wireless environments, when signal coverage needs to be analyzed over large areas with fine discretization.

Fig. 7 Indoor simulation methods in Altair WinProp: Multi-Wall Model (left), Standard Ray Tracing (center) and Dominant Path Model (right). 

Standard Ray Tracing (Fig. 7, center) follows a much more rigorous approach, in which many ray paths between transmitter and receiver are analyzed. These include rays with multiple reflections, transmissions, edge diffractions and combinations of all these mechanisms. There would be more rays than those drawn in the image. This method has the advantage of accuracy, but at the expense of computational time. Especially when the number of diffractions in a ray path increases, the speed decreases, because at each diffraction many new rays are spawned. As a consequence, one rarely includes more than two diffractions in practice. In a complicated indoor environment over distances that are not short, one needs to include more diffraction, so the accuracy suffers.

The Dominant Path Model (Fig. 7, right) [14] offers, for a complicated indoor environment, the best accuracy in a reasonable time. This proprietary method determines rapidly which path between transmitter and receiver is likely to be the dominant one, i.e. likely to carry the bulk of the signal power. This path can have any combination of transmissions, reflections and diffractions, thus the received signal is calculated rapidly. Since more diffraction can be included than in Standard Ray Tracing, the Dominant Path Model has higher accuracy in complicated indoor environments for receiver positions not close to the transmitter.

Figs. 8 and 9 display the computational results obtained with Altair WinProp™ of the signal over the entire second floor at 28 and 38 GHz. Table IV presents the experimental measurements of path loss in the paths indicated in Figs. 8 and 9 and the estimated propagation coefficients of each path. Note the variation in the propagation coefficients that were estimated from the measurements. This variation reflects the line-of-sight conditions, as it might also be observed in the computational results from Figs. 8 and 9: the smallest value occurs for trajectory 1 (line of sight), the second-smallest for trajectory 2 (obstructed line-of-sight but no walls to penetrate), while the largest values occur for trajectories that penetrate several walls. The values of the propagation coefficient vary from 3.85 to 4.57, whereas the received power estimated was from −178 to −60 dBm. Knowledge of these values and insight in the factors that determine them can help to quickly assess wireless coverage in an indoor environment.

Table IV REFLECTION COEFFICIENTS 

Path Frequency n σ¯(dB) σmax(dB) Distance (m)
1 28 2.86 8.4 11.1 67
38 2.92 9.4 12.2 67
2 28 3.42 9.4 12.6 38
38 3.51 8.6 11.4 38
3 28 3.85 9.5 12.9 58
38 4.11 6.6 9.7 58
4 28 4.57 8.7 12.5 88

Fig. 8 Numerical simulation of the coverage map at 28 GHz an indoor environment. 

Fig. 9 Numerical simulation of the coverage map at 38 GHz an indoor environment. 

IV. Conclusions

We have characterized the reflection and transmission coefficients of several building materials in mm-waves. Furthermore, we have demonstrated the path losses in an indoor environment follow a log-distance propagation model of which the propagation coefficient can be determined. This methodology enables a rapid assessment of wireless coverage in general indoor environments. A more detailed comparison with simulated results, for a wider variety of environments, will be performed as a future work. such a study is expected to lead to better insight in uncertainties and correction factors, if any, to be taken into account. Armed with this insight, eventually a sophisticated radio planning in a wide variety of environments will be possible without the need for extensive measurements. As a final conclusion, the obtained results contribute to the planning of the future 5G networks, operating in mm-waves.

V. References

1. [1] Cisco Systems Inc., “Cisco Visual Networking Index: Global Mobile Data Traffic Forecast Update, 2016-2021,” White Paper, Feb. 2017. [ Links ]

2. [2] ITU-R, “M.2370-0 IMT traffic estimates for the years 2020 to 2030,” 2015. [ Links ]

3. [3] Attenuation by atmospheric gases, ITU-R Standard P.676-11,2016. [ Links ]

4. [4] Specific Attenuation model for rain for use in prediction methods, ITU-R Standard P.838-3, 2005. [ Links ]

5. [5] T. S. Rappaport, G. R. MacCartney, M. K. Samimi, and S. Sun, “Wideband Millimeter-Wave Propagation Measurements and Channel Models for Future Wireless Communication System Design,” IEEE Transactions on Communications, v. 63, n°. 9, pp. 3029-3056, Sep. 2015. [ Links ]

6. [6] H. Zhao, R. Mayzus, T. S. Rappaport, “28 GHz Millimeter Wave Cellular Communication for Reflection and Penetration Loss in and around Buildings in New York City,” IEEE Wireless Communications Symp., pp. 5163-5167, Jun. 2013. [ Links ]

7. [7] O. Landron, M. J. Feuerstein, T. S. Rappaport, “In Situ Microwave Reflection Coefficient Measurements for Smooth and Rough Exterior Wall Surfaces,” IEEE Vehicular Technology Conference, May. 1993. [ Links ]

8. [8] G. R. Maccatney, J. Zhang, S. Nie, T. S. Rappaport, “Path Loss for 5G Millimeter Wave Propagation Channels in Urban Microcells,” IEEE Global Communications Conference, Dec. 2013. [ Links ]

9. [9] C. C. Pu, S.Y. Lim, P. C. Ooi “Measurement Arrangement for the Estimation of Path Loss Exponent in Wireless Sensor Network” IEEEComputing and Convergence Technology (ICCCT), Dec. 2012. [ Links ]

10. [10] M. H. Sunil Srinivasa, “Path loss exponent estimation in large wireless networks” Information Theory and Applications Workshop, Feb. 2009. [ Links ]

11. [11] G. L. Yongchang Hu, “Self-Estimation of Path-Loss Exponent in Wireless Networks and Applications” IEEE Transactions on Vehicular Technology, vol. 64, no. 11, Nov. 2015. [ Links ]

12. [12] WallMan for Windows, version 14.1: WinProp. Altair Engineering, Inc. 2017. [ Links ]

13. [13] AMan for Windows, version 14.1: WinProp. Altair Engineering, Inc. 2017. [ Links ]

14. [14] ProMan for Windows, version 14.1: WinProp. Altair Engineering, Inc. 2017. [ Links ]

Received: October 04, 2018; Revised: November 09, 2018; Accepted: November 20, 2018

Creative Commons License This is an Open Access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.