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Journal of Microwaves, Optoelectronics and Electromagnetic Applications

On-line version ISSN 2179-1074

J. Microw. Optoelectron. Electromagn. Appl. vol.11 no.1 São Caetano do Sul June 2012

http://dx.doi.org/10.1590/S2179-10742012000100013 

Analysis of microstrip antennas on carbon fiber composite material

 

 

Rodrigo R. de AssisI; Ildefonso BianchiII

IDepartment of Electronic and Computer Engineering, Instituto Tecnológico de Aeronáutica, São José dos Campos – SP, Brazil, r2.assis@gmail.com
IIDepartment of Electronic and Computer Engineering, Instituto Tecnológico de Aeronáutica, São José dos Campos – SP, Brazil, ibianchi@ita.br

 

 


ABSTRACT

In this paper a truncated corner rectangular microstrip antenna (TCRMA) is analyzed in the presence of carbon fiber composite (CFC) material. Simplified carbon fiber composite models are proposed and the analyses are performed by the electromagnetic simulator Computer Simulation Technologies (CST). Theoretical and experimental results of return loss, axial ratio, input impedance and radiation pattern for the antenna located on the aluminum and CFC plates are presented and compared. The results show that the proposed models can be used as a good approximation of the CFC sample and that the CFC material is a feasible alternative instead of aluminum for antenna applications on complex structures such as ships or airplanes.

Index Terms: Carbon fiber composite (CFC), microstrip antenna.


 

 

I. INTRODUCTION

The search for new improved materials that could replace the aluminum or other conductors is a common task for many applications in the aerospace industry. Weight reduction, more tolerance to fatigue and easiness of construction for complex structures are some advantages of using such materials. These characteristics can lead to operational costs reduction and performance increase. The carbon fiber composite (CFC) is a successful and well-know example of such materials in many applications. Several studies have been made in recent years to analyze the CFC electrical properties [1]-[5]. However, some technical aspects still aren't fully explored by the scientific community, such as the antenna behavior in the presence of these materials. There are several antenna topologies that require a conductive ground plane in order to properly operate, and the knowledge of their behavior in such environment is important to establish an optimal operational condition.

This paper presents theoretical analyses to evaluate the figures of merit of a circular polarized truncated corner rectangular microstrip antenna (TCRMA), which is designed to operate in the satellite navigation frequency range, in the presence of the CFC material. The approach is to consider a fictitious custom-off-the-shelf (COTS) antenna and analyze it on a CFC ground plane as this is considered a practical situation. The trend in the aerospace industry is the replacement of certain structural parts by composite materials [6], and the analysis of these materials at high frequencies using numerical techniques requires great computational effort as the dimensions are electrically large [7]. Thus, the search for faster and more accurate solutions is still a challenge, mainly considering the possibility of analyses on larger structures such as ships or airplanes. Theoretical results are compared with experimental ones for CFC and aluminum samples.

 

II. DESCRIPTION OF CFC MATERIAL

There are many ways to configure a composite material, such as concentration percentage, shape and size of the components. The CFC material sample used in the experiments is formed by clusters of carbon fiber immersed in epoxy resin. It is composed by 60 % of carbon fibers and 40 % of resin. The fibers are continuous and have a cylindrical format with 7.1 µm diameter. Each set contains 12000 fibers with a total cross section area of 0.48 mm2. The material contains ten layers with thickness of 0.21 mm, where the first and last two layers are arranged in the orientation [0º, 90º] and the remaining ones are arranged in the orientation [45º, -45º], as illustrated in Fig. 1.

 

 

Due to the complexity of modeling the real geometry, witch requires a great computational effort, the theoretical analyses are made using two simplified models of the CFC plate. Moreover, comparisons with experimental results are made to validate the proposed simplification. In the first model (CFC[a]) the electrical conductivity and effective permittivity of the material are estimated through the law of mixtures [8], [9]

where P indicates electrical permittivity (ε) or conductivity (σ), v is the percentage of carbon in the CFC, the indexes carb and res denote parameters of carbon and resin, and the index eff denotes the effective parameters of the CFC. Considering the relative permittivities εres = 4.0 and εcarb = 12.0, the electric conductivities σres = 0 and σcarb = 1.0 x 105 S/m, and the percentage of carbon v = 0.6, it is obtained εeff = 8.8 and σeff = 5.9 x 104 S/m. Thus the CFC[a] model is considered a homogeneous material with the above shown effective parameters, relative magnetic permeability µr = 1 and null loss tangent. The second model (CFC[b]) consists of carbon strips embedded in epoxy resin, as illustrated in Fig. 2, which represents one layer of the material used in the experiments. The carbon strips are spaced 2.2 mm and have a rectangular cross section of 2.2 x 0.1 mm. The carbon material is modeled with εcarb = 12, µr = 1 and σcarb = 1 x 105 S/m, and the epoxy resin layer has a thickness of 0.202 mm, εres = 4 and null loss tangent.

 

 

III. MICROSTRIP ANTENNA BEHAVIOR IN THE PRESENCE OF CFC MATERIAL

The placement of a COTS antenna on a large structure is a common situation in the aerospace industry. In this case the antenna is usually designed on a flat ground plane and its behavior is expected to be similar when installed on large complex structures. In new applications these structures are being replaced by composite materials due to their mechanical benefits and the behavior of an antenna installed on these materials can be a challenging task in many aspects, such as mechanical installation, lightning protection or static discharge. Besides, the behavior of antennas' figures of merit is also not fully explored in the scientific community. In order to evaluate these features it is chosen a circular polarized microstrip antenna with truncated corners, as depicted in Fig. 3. This antenna was chosen due to its narrow bandwidth considering both the circular polarization and the input impedance, as any small change in the antenna surroundings can influence these tune features.

 

 

The antenna is designed on a 30 x 30 cm aluminum plate, as shown in Fig. 3, to operate at the center frequency of 1575 MHz and with right-hand circular polarization. The substrate is Arlon CuCLAD 250GX with a thickness of 3.048 mm, εr = 2.55 and loss tangent of 0.0018. The dimensions of the antenna are: W = 85.0 mm, L1 = 57.9 mm, L2 = 57.3 mm, C = 6.2 mm, p = 16.5 mm. The antenna has its own conductive ground plane limited by the substrate dimensions (W) and the material under test (CFC and aluminum) is positioned below it, as shown in Fig. 3.

The theoretical analysis is performed by the CST simulator, where the frequency domain was used for the CFC[a] model and the time domain was used for the CFC[b] model. The input impedance and return loss measurements were made using the vector network analyzer HP 8714ET in the Antenna and Propagation Laboratory at Instituto Tecnológico de Aeronáutica (ITA) and the axial ratio and radiation pattern measurements were performed in the anechoic chamber of Instituto de Fomento Industrial (IFI), both part of Departamento de Ciência e Tecnologia Aeroespacial (DCTA), as shown in Figs. 4 and 5.

 

 

 

 

The theoretical and experimental results of return loss, axial ratio, input impedance and radiation pattern for the antenna located on the aluminum and CFC plates are shown in Figs. 6 and 7.

The results of axial ratio and return loss for the TCRMA antenna without the 30 x 30 cm plate are also shown in Fig. 6 (a) and Fig. 7 (b). From these results it can be concluded that the antenna features are degraded in the condition without the plate.

As presented in Fig. 6 (a), the theoretical axial ratio results for the CFC plate are similar to the theoretical values obtained for the aluminum plate. The small difference between these values doesn't change the condition of circularly polarized antenna. Similarly the experimental results do not present significant variation comparing the aluminum and the CFC plates. The small displacement between the points of best axial ratio, when comparing theoretical values with experimental ones, is within the substrate material tolerances provided by the manufacturer and it corresponds to 0.09% of the design frequency. It was also noted that this difference does not compromise the correct operation of the antenna. The radiation pattern in the yz plane at the frequency of 1576.5 MHz is shown in Fig. 6 (b). The maximum difference between theoretical and experimental results was approximately 0.2 dB. These results indicate that the radiation pattern is not significantly changed when replacing the aluminum plate by CFC plate.

The input impedance results considering the aluminum and CFC plates were also similar, as shown in Fig. 7 (a). The maximum percentage deviation at the frequency of 1575 MHz was 0.1% (CFC[a]), 11.7% (CFC[b]) and 1.8% (measured CFC sample), considering the reference being the antenna on the aluminum plate. In Fig. 7 (b) it is noted that the CFC[a] model exhibited a return loss similar to the theoretical model of the aluminum plate and both had a deviation of about 11 dB at 1575 MHz compared to measured results. The CFC[b] model presented a deviation of about 4 dB from measured values at 1575 MHz. However, as these results were below 22 dB, it can be concluded that replacing the aluminum plate by CFC plate does not significantly degrade the return loss of the antenna.

The theoretical antenna gain results for aluminum and CFC plates in the yz plane at 1576.5 MHz are shown in Fig. 8. The gain for the three material models is about 6 dBi and its variation is less than 2%. Thus, it is concluded that the use of CFC plate does not degrade significantly the antenna efficiency in comparison to the aluminum plate. This result emphasizes the advantage of keeping the metallic antenna ground plane underneath its substrate.

 

 

IV. CONCLUSIONS

The analysis of composite materials at high frequencies using numerical techniques requires large computational effort, making the search for faster and more accurate solutions a challenge, mainly considering the possibility of analyses on larger structures such as ships or airplanes. This paper presented theoretical and experimental analysis of the TCRMA's figures of merit in the presence of a carbon fiber composite sample, where simplified material models were proposed in order to reduce the computational effort. The agreement between theoretical and experimental results shows that the proposed CFC material models can be used as a good approximation of the CFC sample, enabling analyses of antennas in the presence of more complex and electrically large structures such as airplanes. In addition, the expected performance of the CFC material is similar to the performance of aluminum under the studied conditions. Thus, it can be concluded that the CFC material is a feasible alternative instead of aluminum for antenna applications on complex structures such as ships or airplanes.

 

REFERENCES

[1] C.P. Neo and V.K. Varadan, Design and development of electromagnetic absorbers with carbon fiber composites and matching dielectric layers, IOP Electronic Journals, Smart Materials and Structures, October 2001.         [ Links ]

[2] S. Bhattacharya, V.K. Sachdev and R.P. Tandon, Electrical properties of graphite filled polymer composites, 2nd National Conference Mathematical Techniques: Emerging Paradigms for Electronics and IT Industries, September 2008.         [ Links ]

[3] A. Cîrciumaru, G. Andrei, I.G. Bîrsan and D. Dima, Electric and electromagnetic properties of fiber fabric based filled epoxy composites, The Annals of "Dunarea De Jos" University of Galati, Fascicle IX. Metallurgy and Materials Science, nº 2, pp. 26-28, ISSN 1453, 2007.         [ Links ]

[4] I.M. Rosa, F. Sarasini, M.S. Sarto and A. Tamburrano, EMC impact of advanced carbon fiber/carbon nanotube reinforced composites for next-generation aerospace applications, IEEE Transactions on Electromagnetic Compatibility, vol. 50, nº.3, pp. 556-562, August 2008.         [ Links ]

[5] A. Mehdipour, A.-R. Sebak, C. W. Trueman, I. D. Rosca, and S. V. Hoa, "Performance of microstrip patch Antenna on a reinforced carbon fiber composite ground plane," Microwaves and Optical Technology Lett., vol. 53,no. 6, pp. 1328-1331, 2011.         [ Links ]

[6] SAE International, CNC fiber placement used to create an all-composite fuselage, Aerospace Engineering & Manufacturing Online, available in: www.sae.org/aeromag/techinnovations/1298t08.htm, access in: April 13, 2010.         [ Links ]

[7] R.R. de Assis, I. Bianchi and R. Schildberg, Análise de antenas sobre compósito de fibra de carbono para aplicações em aeronaves, 14th Simpósio Brasileiro de Microondas e Optoeletrônica and 9th Congresso Brasileiro de Eletromagnetismo, Vila Velha -ES, August 2010.         [ Links ]

[8] S.E. Lee, K.S. Oh and C.G. Kim, Electromagnetic characteristics of frequency selective fabric composites, IEEE Electronic Letters, vol. 42, issue 8, pp. 439-441, April 2006.         [ Links ]

[9] S. Rea, D. Linton, and. Or e J. McConnel, Electromagnetic shielding properties of carbon fibre composites in avionic systems, Microwave Review, June 2005.         [ Links ]

 

 

Received 7 Nov. 2011; for review 14 Nov. 2011; accepted 15 June 2012