Research Article  Open Access
Impacts of Absorber Loadings on Simulating the Multipath Channel in a Reverberation Chamber
Abstract
In reverberation chambers, the multipath channels with different delay characteristics can be generated by loading the chamber with different amounts of absorbers. This paper investigates the impacts of absorber loadings on the delay characteristics based on realistic measurements. An efficient method for estimating the rootmeansquare (rms) delay spread in the chamber is presented. Furthermore, it is found that the chamber loadings also significantly affect the quality of a digitally modulated signal and the corresponding modulation quality measurements are performed.
1. Introduction
Reverberation chambers (RCs) are traditionally used for electromagnetic compatibility (EMC) measurements [1, 2], and during the past decade this test facility has also attracted a lot of attentions in the wireless communication field [3–5]. In such applications, the RC is used to simulate a multipath channel. The RC is basically a metal cavity that is stirred to emulate the channel [6].
The channel characteristics in the RC have been studied in many works [7–11]. For example, Genender et al. [7] showed how the power delay profile can be measured and controlled inside a RC, and it was shown that changing the loading influences the power delay profile. In [8, 9], rootmeansquare (rms) delay spread was measured inside a RC with different amounts of absorber. The measured results were compared with those obtained in some realworld environments. The papers demonstrated that it is possible to simulate various realworld environments inside the RCs by changing the loadings. In [10, 11], theoretical derivation of the relationship of rms delay spread and coherence bandwidths in RC was presented. To verify the theoretical results, measurements in a RC with different loadings were conducted. All these papers showed that the channel characteristics can be adjusted by loading chamber, and some papers, for example, [8, 11], have qualitatively described the relation between the rms delay spread and the amounts of absorbing objects; that is, adding absorber will shorten the rms delay spread. However, in some applications, for example, overtheair (OTA) test, the delay spread of the channels in the RC significantly affects the test results. Then here is one question: what is the accurate quantitative relation between the amounts of absorbers and the rms delay spread in the RC? This problem has not been well solved in the existing literatures.
The absorber loading has a significant impact on the rms delay spread of the generated channel and thus affects the signal quality. Some papers have studied the impact of absorber loading on the bit error rate (BER) [8, 12]; however, modulation quality parameters, for example, Error Vector Magnitude (EVM), as alternative metrics offer several advantages. Firstly, measurements of EVM and related modulation quality parameters can pinpoint the type of degradations in a signal [13, 14]. Secondly, the BER measurement relying on the Monte Carlo approach has a long measurement time, especially at low BERs [8]. By contrast, the modulation quality parameters can be readily evaluated by transmitting fewer symbols, as compared to the BER. Hence, characterizing the performance using modulation quality parameters is preferred. However to the best of the authors’ knowledge, little work has been conducted to address the impact on the modulation quality parameters. This paper aims to fill this gap.
The main contributions of this paper may be summarized as follows:(1)An efficient method to accurately estimate the rms delay spread in the RC with amounts of absorbers is presented.(2)The influences of heavy loading on the variance of the rms delay spread in the RC are discussed.(3)The effect of the absorber loading on the modulation quality of a digitally modulated signal is investigated.
2. Impact on rms Delay Spread
The rms delay spread is widely used to characterize the delay dispersion of the channel [15]. To study the effects of the absorber loading on the rms delay spread, we used the measurement system as shown in Figure 1. The test chamber was the National Institute of Metrology (NIM) reverberation chamber, having a dimension of 5.09 m 6.43 m 5.57 m, as shown in Figure 2. The large size yields a generated channel with large rms delay spread and is suitable for replicating environments with a large number of multipath components, for example, urban environments [16]. The transmitting antenna was a horn antenna directed into a corner of the chamber, and the receiving antenna was a biconical antenna placed in the middle of the RC. The mechanical stirring was performed by two metal plates that were moved stepwise. We used two sizes of absorbers. As shown in Figure 3, for the small one, each piece is with 6 cones in a array, the cone width is 10.2 cm, and the cone height is 30.5 cm. For the large one, each piece is with 81 cones in a array, the cone width is 6.8 cm, and the cone height is 17.8 cm.
(a)
(b)
Measurements were conducted in the frequency domain by measuring the channel transfer function (CTF) over a frequency ranging from 4.9 GHz to 5.1 GHz, using the vector network analyzer (VNA) based measurement system as shown in Figure 1 [17]. We can get the empirical channel impulse responses (CIRs), , by performing an inverse fast Fourier transform algorithm () of the measured CTF, , as [17]and the CIR can be expressed aswhere , , and denote the amplitude, phase, and delay of the th multipath component (MPC), respectively, is the total number of MPCs, and is the Dirac delta function. The power delay profile (PDP) of the channel is defined as the square magnitude of the CIR as follows:
Then the rms delay spread can be calculated aswhere and represent the delay and corresponding delay power of the ith MPC measured, respectively. When computing the rms delay spread, we set the power of all the MPCs below a threshold to zero to reduce the impact of the noise. The threshold is set to be 6 dB above the noise floor [18].
The measurement was repeated for 100 different fixed paddle positions spaced by . The large number of paddle positions provides sufficient measurement data for the analysis of the variance of the rms delay spread. For the rms delay spread estimation, the 100 measurement results were averaged to obtain the mean values for various amounts of absorbers. To show the variance of the rms delay spread, the maximum, minimum, standard deviation (SD), and relative standard deviation (RSD, equal to SD/mean) of the rms delay spread are also summarized in Table 1.

It has been shown that the rms delay spread is directly related to the chamber quality factor by the following [8]:where is the carrier frequency and the quality factor, , is the proportion of energy stored to the energy dissipated. The value of , that is, in (6), is given by [19]where is associated with the wall loss, is associated with energy dissipated in the antenna, and is associated with absorber loss. This paper focuses on the relation between the number of absorbing objects and the generated rms delay spread. Then (6) is rewritten aswhere equals and the subscript “” of indicates the number of absorbers. The combination of (5) and (7) makes it possible to relate the number of absorbers and the rms delay spread; that is,where is the rms delay spread for the RC with absorbers, that is, the mean values in Table 1. is the rms delay spread for the RC with unloading.
Then (equal to ) can be calculated from the measurement results. The calculated is shown in Figure 4. By fitting the experimental data with a least squares regression curve, a linear model is suggested:
The combination of (8) and (9) yieldswhere (10), the rms delay spread for the RC (mean value) with absorbers, , can be estimated. In the model of (10), and can be obtained from the measurements with unloading and one loading in the RC, respectively. In our measurements, (ns); and for the large absorber case, (ns), and for the small absorber case, (ns).
For the proposed model of (10) applied to all the chamber loadings in Table 1, the estimated relative error for absorbers can be calculated aswhere is the estimated rms delay spread for absorbers and is the measured rms delay spread, that is, the mean values in Table 1. In Table 1, for different numbers of absorbers was also listed. The mean relative error is 2.52%. The maximum relative error is 4.02% corresponding to the four large absorbers loaded, which is more accurate compared with other methods [19].
Furthermore, in Table 1, we find that SD and RSD increase monotonically with the increasing amount of absorbers for both the large absorbers and small absorbers. A potential explanation is that the heavy loading decreases the uniformity in the RC and leads to the variance of the rms delay spread. The decrease of uniformity also increases the measurement uncertainty. As suggested in [20, 21], the intrinsic field uncertainty (IFU) associated with random fields inside the RC is the major contribution to the overall measurement uncertainty and the IFU at receiver can be evaluated as [20]where is number of paddle positions, that is, the average number. In our measurements, the maximum is 7.4 ns corresponding to the four large absorbers loaded, which is much less than the measurement results (the mean values in Table 1).
3. Impact on Modulation Quality
In order to investigate the impact of chamber loading on the quality of digitally modulated signals, we carried out modulation quality measurements inside the RC with different loadings.
EVM is a key measure used to quantify the performance of a digital signal [13, 22]. An ideal signal would have all constellation points precisely at the ideal locations; however various imperfections including the influence of channel characteristics cause the actual constellation points to deviate from the ideal locations. Figure 6 shows a vectorial representation using the constellation diagram. The error vector between the ideal complexvalued symbol and the received symbol is defined as . For our measurements, a total number of 1000 symbols are measured, and then can be expressed as follows:where is average symbol power and is number of measured symbols. As one of the most important modulation quality parameters, has been used to study the effects of the physical propagation channel on a digitally modulated signal [14, 23].
The measurement setup for obtaining the EVM is shown in Figure 5. A vector signal generator (VSG) was used to generate the Quadrature Phase Shift Keying (QPSK) signals with different symbol rates (15 ks/s and 60 ks/s). The output power of the VSG was 10 dBm. The center frequency of the modulated signals was 5 GHz. Up to four large absorbers were used to investigate the impact of the chamber loading on the modulation quality. A vector signal analyzer (VSA) was used to receive waveforms, demodulate them, and measure the modulation quality. Again, we placed a horn antenna directed into a corner as the transmitting antenna and a discone antenna in the middle of the RC as the receiving antenna. The measurement was also repeated for 100 different fixed paddle positions as the rms delay spread measurements.
Before conducting the measurements in the RC, modulation quality measurements were performed with connecting the VSA and VSG directly with a cable, where is found to be 0.25% and 0.27% for 15 ks/s and 60 ks/s, respectively. The low residual errors enable the study of RCinduced effects rather than receiverinduced effects on the modulation quality.
The measurement results of the mean values of are shown in Figure 7. Firstly, it can be seen that low symbol rate leads to a better modulation quality. The lower symbol rate essentially implies a narrower bandwidth, which is less sensitive to frequency selectivity of channel. This is the reason that the signal with lower symbol rate will degrade less for given absorbers. Furthermore, as shown in Figure 7, heavy loading leads to better modulation quality. As mentioned above, heavy loading leads to smaller delay spread. It has been shown that the coherence bandwidth (as the measure of the frequency selectivity) is reversely proportional to the rms delay spread [10, 11]. Therefore, adding absorber will widen the coherence bandwidth and finally leads to better modulation quality [12].
As observed in Figure 7, the mean value of fits to a rational function well, which can be written aswhere indicates the number of absorbers. and are the coefficients for the rational function. For the symbol rate of 15 ks/s, and ; for the symbol rate of 60 ks/s, and . Note that this model is heuristic, whose ultimate justification lies in its ability to fit the measurement data.
Table 2 shows the statistics of . It is found that the SD and RSD are considerably high. The reason is that values at some paddle positions are much higher than the mean values; for example, see column Max in Table 2. The high values may come from the fact that the reflected signals cause the receiver to experience a severe fading at some paddle positions. The modulation quality of the digitally modulated signals in the RC is sensitive to the paddle positions.

The EVM is the total error and contains various degradations [13]. In order to pinpoint the degradations, four main modulation quality parameters, that is, magnitude error (ME), phase error (PE), gain imbalance (GI), and quadrature imbalance (QI) [13, 14], were measured with the same measurement setup as the EVM measurement. Figure 8 shows the mean values over the 100 paddle positions of these modulation quality parameters for different loadings. It is found that heavy loading decreases the magnitude error and phase error but the quadrature imbalance and gain imbalance do not decrease monotonically with the amount of absorbers.
(a)
(b)
(c)
(d)
4. Conclusions
This paper investigates the impacts of the absorber loadings on the delay spread and modulation quality in the RC. Based on the measurements, an efficient method for estimating the rms delay spread in the RC with the amounts of absorbing objects is presented. In addition, it is found that heavy loading leads to an increase of the variance of the rms delay spread in the chamber.
The chamber loadings are found to affect the quality of the digitally modulated signals due to different channel conditions of the generated multipath channels. The modulation quality measurements show that heavy loading leads to a better modulation quality and the modulation quality is sensitive to the paddle positions.
This paper presents implementationspecific details necessary for the use of RCs. Our analysis is based on realistic measurements, which makes the conclusion sufficiently reliable and can be applied when using a RC to simulate wireless propagation environments.
Conflicts of Interest
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgments
This work was supported in part by the National Key Technology R&D Program under Grants 2014BAK02B05 and 2014BAK02B04; by the Natural Science Base Research Plan in Shanxi Province of China under Grant 2015JM6320; by National Natural Science Foundation of China under Grant 61501020; by State Key Laboratory of Rail Traffic Control and Safety under Grants RCS2016ZJ005 and RCS2015ZZ001; by China Postdoctoral Science Foundation under Grant 2016M591355; by Fundamental Research Funds for the Central Universities under Grant 2016JBZ006; and by the National 863 Key Project under Grant 2014AA01A706. The authors would like to thank Dr. Kate A. Remley and Qiulai Gao for their helpful suggestions and support. The authors also thank S. Ding and Y. Liu for their assistance during the preparation of the measurement campaign.
References
 C. L. Holloway, D. A. Hill, M. Sandroni et al., “Use of reverberation chambers to determine the shielding effectiveness of physically small, electrically large enclosures and cavities,” IEEE Transactions on Electromagnetic Compatibility, vol. 50, no. 4, pp. 770–782, 2008. View at: Publisher Site  Google Scholar
 C. L. Holloway, D. A. Hill, J. Ladbury, G. Koepke, and R. Garzia, “Shielding effectiveness measurements of materials using nested reverberation chambers,” IEEE Transactions on Electromagnetic Compatibility, vol. 45, no. 2, pp. 350–356, 2003. View at: Publisher Site  Google Scholar
 X. Chen, B. P. Einarsson, and P.S. Kildal, “Improved MIMO throughput with inverse power allocation—study using USRP measurement in reverberation chamber,” IEEE Antennas & Wireless Propagation Letters, vol. 13, no. 13, pp. 1494–1496, 2014. View at: Publisher Site  Google Scholar
 R. Recanatini, F. Moglie, and V. M. Primiani, “Performance and immunity evaluation of complete wlan systems in a large reverberation chamber,” IEEE Transactions on Electromagnetic Compatibility, vol. 55, no. 5, pp. 806–815, 2013. View at: Publisher Site  Google Scholar
 S. J. Floris, K. A. Remley, and C. L. Holloway, “Bit error rate measurements in reverberation chambers using realtime vector receivers,” IEEE Antennas and Wireless Propagation Letters, vol. 9, no. 1, pp. 619–622, 2010. View at: Publisher Site  Google Scholar
 P. Corona, G. Ferrara, and M. Migliaccio, “Reverberating chamber electromagnetic field in presence of an unstirred component,” IEEE Transactions on Electromagnetic Compatibility, vol. 42, no. 2, pp. 111–115, 2000. View at: Publisher Site  Google Scholar
 E. Genender, C. L. Holloway, K. A. Remley, J. Ladbury, G. Koepke, and H. Garbe, “Use of reverberation chamber to simulate the power delay profile of a wireless environment,” in Proceedings of the IEEE International Symposium on Electromagnetic Compatibility (EMC '08), pp. 1–6, September 2008. View at: Publisher Site  Google Scholar
 E. Genender, C. L. Holloway, K. A. Remley, J. M. Ladbury, G. Koepke, and H. Garbe, “Simulating the multipath channel with a reverberation chamber: application to bit error rate measurements,” IEEE Transactions on Electromagnetic Compatibility, vol. 52, no. 4, pp. 766–777, 2010. View at: Publisher Site  Google Scholar
 S. Herbert, T.H. Loh, I. Wassell, and J. Rigelsford, “On the analogy between vehicle and vehiclelike cavities with reverberation chambers,” IEEE Transactions on Antennas and Propagation, vol. 62, no. 12, pp. 6236–6245, 2014. View at: Publisher Site  Google Scholar  MathSciNet
 X. Chen, P.S. Kildal, C. Orlenius, and J. Carlsson, “Channel sounding of loaded reverberation chamber for overtheair testing of wireless devices: coherence bandwidth versus average mode bandwidth and delay spread,” IEEE Antennas and Wireless Propagation Letters, vol. 8, pp. 678–681, 2009. View at: Publisher Site  Google Scholar
 X. Chen and P.S. Kildal, “Theoretical derivation and measurements of the relationship between coherence bandwidth and RMS delay spread in reverberation chamber,” in Proceedings of the 3rd European Conference on Antennas and Propagation (EuCAP '09), pp. 2687–2690, Berlin, Germany, March 2009. View at: Google Scholar
 K. A. Remley, S. J. Floris, H. A. Shah, and C. L. Holloway, “Static and dynamic propagationchannel impairments in reverberation chambers,” IEEE Transactions on Electromagnetic Compatibility, vol. 53, no. 3, pp. 589–599, 2011. View at: Publisher Site  Google Scholar
 J. L. Pinto and I. Darwazeh, “Error vector magnitude relation to magnitude and phase distortion in 8PSK systems,” Electronics Letters, vol. 37, no. 7, pp. 437–438, 2001. View at: Publisher Site  Google Scholar
 V. A. Thomas, S. Kumar, S. Kalyani, and M. ElHajjar, “Error vector magnitude analysis of fading SIMO channels relying on MRC reception,” IEEE Transactions on Communications, vol. 64, no. 4, pp. 1786–1797, 2016. View at: Publisher Site  Google Scholar
 P. A. Bello, “Characterization of randomly timevariant linear channels,” IEEE Transactions on Communications Systems, vol. 11, no. 4, pp. 360–393, 1963. View at: Publisher Site  Google Scholar
 J. Laurila, K. Kalliola, M. Toeltsch, K. Hugl, P. Vainikainen, and E. Bonek, “Wideband 3D characterization of mobile radio channels in urban environment,” IEEE Transactions on Antennas & Propagation, vol. 50, no. 2, pp. 233–243, 2002. View at: Publisher Site  Google Scholar
 X. Zhou, Z. Zhong, B. Zhang et al., “Experimental characterization and correlation analysis of indoor channels at 15 GHz,” International Journal of Antennas and Propagation, vol. 2015, Article ID 601835, 11 pages, 2015. View at: Publisher Site  Google Scholar
 A. F. Molisch and M. Steinbauer, “Condensed parameters for characterizing wideband mobile radio channels,” International Journal of Wireless Information Networks, vol. 6, no. 3, pp. 133–154, 1999. View at: Publisher Site  Google Scholar
 D. A. Hill, M. T. Ma, A. R. Ondrejka, B. F. Riddle, M. L. Crawford, and R. T. Johnk, “Aperture excitation of electrically large, lossy cavities,” IEEE Transactions on Electromagnetic Compatibility, vol. 36, no. 3, pp. 169–178, 1994. View at: Publisher Site  Google Scholar
 IEC, “Electromagnetic compatibility (EMC)part 4–21: testing and measurement techniquesreverberation chamber test methods,” Tech. Rep. IEC 61000421, 2003. View at: Google Scholar
 L. R. Arnaut, “Measurement uncertainty in reverberation chambersI. Sample statistics,” NPL Report TQE 2, National Physical Laboratory, Teddington, UK, 2008. View at: Google Scholar
 A. Georgiadis, “Gain, phase imbalance, and phase noise effects on error vector magnitude,” IEEE Transactions on Vehicular Technology, vol. 53, no. 2, pp. 443–449, 2004. View at: Publisher Site  Google Scholar
 C. Jastrow, S. Priebe, B. Spitschan et al., “Wireless digital data transmission at 300 GHz,” Electronics Letters, vol. 46, no. 9, pp. 661–663, 2010. View at: Publisher Site  Google Scholar
Copyright
Copyright © 2017 Xin Zhou et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.