# Iterative Full-Wave Analysis of Mandelbrot-Inspired Fractal Patch Antenna on Textile Substrate for UWB Applications

Authors: V. P. Silva Neto; A. G. D’Assunção
Journal: International Journal of Antennas and Propagation
 (2017)

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## Abstract

This work presents the analysis of monopole microstrip antennas with truncated ground plane and patch geometry inspired on the Mandelbrot fractal curve for applications in UWB systems. The proposed antenna geometry is analyzed using the Wave Concept Iterative Procedure (WCIP), a full-wave method. Results for the proposed antenna operating frequency, bandwidth, VSWR, gain, and radiation pattern are obtained and discussed. The WCIP results are compared with simulation results provided by HFSS software, for validation purpose. In addition, a prototype antenna is built and measured. A good match between WCIP theoretical and simulation, HFSS simulation, and measurement results is observed for the antenna frequency response.


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## Body

## 1. Introduction

The continuous advance in wireless communication systems has motivated many researchers worldwide to investigate and develop antennas for ultrawideband (UWB) system applications. The great interest in this particular antenna topic is due to several factors such as immunity to the spreading of multipath, difficulty in accessing signal invader users, less interference when compared to narrowband communications, and low cost. Particularly, microstrip antenna structures are an option of great attractiveness to design UWB antennas with excellent performances.An UWB signal is defined as every signal that occupies a minimum bandwidth of 500 MHz in a particular 7.5 GHz band (from 3.1 GHz to 10.6 GHz), based on the spectral overlap, since much of this spectrum band is used by existing services and technologies [1–3]. Applications of UWB system are very attractive because, due to the required low-power levels, this system can coexist with other technologies operating in the same frequency band networks, such as IEEE 802.11, GSM, and Bluetooth.This paper describes the analysis of a monopole microstrip antenna printed on textile substrate for applications in UWB systems. The use of textile substrate is justified by the increasing need to develop lightweight and flexible devices that could be attached to garments and applied in several areas. For example, several authors have investigated the use of textile substrates, such as microstrip antenna substrates, for applications in biomedical fields [4], surveillance and security systems [5], and telecommunications systems [6].The patch geometry of the proposed antenna is based on the Mandelbrot escape fractal curve [7, 8]. Results for resonant frequency, bandwidth, radiation pattern, and VSWR are obtained using the Wave Concept Iterative Procedure (WCIP). The WCIP is a full wave formulation that has been widely used in recent years in the analysis and characterization of various microwave circuits [9–15].Over the years, several authors have studied the application of fractal geometry in the design of planar antennas and printed antennas for UWB applications [16–18]. In [16], a low-profile compact CPW-fed fractal patch antenna based on a slotted circular shape was proposed for UWB applications. A monopole antenna comprising a fractal radiating patch with folded T-shaped element was designed to operate over the entire UWB frequency range [17]. A miniaturized UWB monopole antenna designed by the combination of two fractal geometries was proposed in [18]. Giusepe Peano and Sierpinski Carpet fractals were used to design the microstrip patch antenna.For comparison purpose, simulations are performed using the finite element method, implemented in the commercial software Ansoft HFSS. In addition, a prototype has been fabricated and measured. Good agreement has been observed between the results obtained by WCIP formulation, HFSS simulations, and experiments.


## 2. WCIP Formulation

The WCIP method is a full-wave iterative method whose formulation is based on the electromagnetic wave concept [9–14]. It is a method that has been widely used by many researchers worldwide in the analysis of different types of microwave circuits such as antennas, filters, and frequency selective surfaces (FSS), including printed circuits on textile substrates, as presented in recent studies [13, 14].The WCIP formulation is based on the relationship between incident and reflected waves at the interface of the circuit under investigation [11]. The relationship between the incident A→ik and reflected B→ik waves is described by the method’s basic equations:
(1)B→ik=S^A→ik+A→01,(2)A→ik=Γ^B→ik,where k (= 1, 2) corresponds to the circuit interface sides 1 (front) and 2 (back). Also, i (= 1, 2, 3, …) represents the order number of the incident A→ik and reflected B→ik waves at the same circuit interface side k. A→01 represents the initial (first) incident wave.The relationship taking place between the incident and reflected waves in front of the circuit interface under analysis is described in (1). Thus, S^ is the “circuit” scattering operator, defined in the space domain and responsible for describing the boundary conditions at the circuit interface [11].The relationship between the incident and reflected waves in the propagation medium apart from the circuit interface under analysis is described in (2). Thus, Γ^ is the “circuit” reflection operator, defined in the modal domain and responsible for describing the propagation characteristics apart from the circuit interface. The determination of the scattering and reflection operators is presented in [11].The iterativity of the WCIP method is obtained using the parameters’ relationships in (1) and (2), which are determined by the transformation between the space and modal domains used in the WCIP formulation. The transition between spatial and modal domains is obtained by applying the Fourier modal transform, for rectangular symmetry type, defined in the following [15].
(3)BmnTEBmnTM=FMTBxi,jByi,j=2δmn/abm2/a+n2/bnb−mamanbFFTBxi,jByi,j,where Bx(i, j) and By(i, j) represent the x and y components, respectively, of the wave in the spatial domain and a and b are the circuit dimensions along the x- and y-axes, respectively; δmn is normalization constant of the orthonormal modal basis for TEmn and TMmn modes that propagate in the rectangular waveguide [15].The Fourier modal transform (FMT) allows you to define the amplitudes of the waves as expansions of TE and TM modes, in the modal domain. This transformation allows the transition of the waves from the spatial domain to the modal domain. The antitransform or inverse Fourier modal transform (FMT−1) allows the return from the modal domain to the spatial domain [11].


## 3. Antenna Design

The antenna structure is shown in Figure1. The antenna patch geometry, shown in Figure 1(a), is inspired on the set of Mandelbrot fractals. The Mandelbrot set, graphically, can be divided into an infinite set of cardioids, with the largest of them located at the center of the complex plane. There is an infinite number of cardioids, which tangentially interconnect the largest cardioid, of many different sizes and whose semimajor axes will tend to zero. Each of these cardioids has its own set of cardioids, whose axes also tend to zero. This process is repeated endlessly, thus generating a Mandelbrot fractal geometry.Figure 1
Mandelbrot monopole patch antenna on textile substrate: (a) antenna patch illustration, (b) antenna structure illustration, and (c) photographs of the fabricated prototype (front and back views).
(a)
(b)
(c)In this work, the Mandelbrot set has been used as a basis to develop the microstrip patch antenna structure. The Mandelbrot sequence has been applied in a circle of radiusR=12.5mm, to generate a quasifractal patch geometry, which can be divided into a set of infinite circles. This patch geometry has been fed by a quarter wavelength microstrip line with characteristic impedance of 50 Ω at the central frequency of the UWB band (6.85 GHz). Figure 1(b) shows the antenna structure considered in this work. The antenna patch is attached on a textile substrate of dimensions 50 mm × 50 mm, with a truncated ground plane to meet the microstrip monopole structure design. Figure 1(c) shows photographs of the front and back views of the fabricated antenna prototype.The brim santista textile material has been used as microstrip substrate, which has the following structural parameters: thicknessh = 1.1 mm, relative permittivity εr = 1.92, and loss tangent tanδ = 0.074 [13]. The patch and ground plane have been fabricated with pure copper polyester taffeta fabric, woven pure copper which is lightweight and flexible and with high conductivity, with a thickness of 0.08 mm and a surface resistance of 0.05 Ohm/sq.


## 4. Results and Discussion

Figure2 shows calculated results using WCIP method for the monopole microstrip Mandelbrot quasifractal geometry with three different substrates: polyester cotton fabric, brim santista textile, and FR4. These results indicate that, at UWB band, the printed monopole antenna on cotton polyester substrate presents return loss values ranging from −17.7 dB (minimum value) to −8.33 dB (maximum value). Therefore, for a −10 dB bandwidth reference, this antenna does not resonate at the entire UWB band. However, it presents a multiband performance, resonating at important operating frequencies such as 2.5 GHz, 2.6 GHz, and 5.8 GHz, used in wireless communication systems. Similarly, the printed monopole antenna on FR4 substrate does not resonate at the entire UWB band. However, unlike the monopole antenna on cotton substrate, it presents a single wideband performance, from 3.93 GHz to 6.93 GHz, useful for particular wireless communication systems.Figure 2
WCIP-simulated return loss results for monopole microstrip antennas on different substrates.In addition, according to the results presented in Figure2, the printed monopole microstrip antenna on brim santista substrate presents return loss values below the −10 dB bandwidth reference within the entire UWB range. Therefore, this antenna can be used in wireless communication systems which operate at the whole UWB range, from 3.1 GHz to 10.6 GHz.To validate the WCIP results presented in Figure2, HFSS simulation and experimental results have been obtained for the printed monopole patch antenna on brim santista substrate. WCIP, HFSS, and measurements return loss and VSWR results, for the monopole antenna on brim santista substrate, are shown in Figures 3(a) and 3(b), respectively, for comparison purpose. Within the whole UWB band, the antenna has presented (WCIP and HFSS) return loss simulated and measured values below −10 dB. In addition, a good agreement between simulation and experimental results is verified. Figure 3(b) exhibits simulated and measured results of the antenna VSWR. Observe that the VSWR values are lower than 2 at the entire UWB band, enabling its use in UWB systems.Figure 3
Frequency responses for fractal monopole microstrip patch antenna on brim santista substrate: (a) return loss and (b) VSWR.
(a)
(b)Considering a maximum value reference of 2 for VSWR and −10 dB for return loss, the obtained simulated and measured results are lower than the reference values over the entire frequency band. In addition, a good agreement between simulation and experimental results is verified for the antenna bandwidth.Figure4 shows the surface current density distribution on the antenna patch. There is a larger current intensity concentrated in the region of the largest circle structure. The determination of the surface current density is very important when wishing to make changes in the structure to control the patch antenna frequency response.Figure 4
Surface current distribution on the fractal patch geometry of the monopole microstrip on brim santista substrate.Figure5 shows 3D and 2D radiation patterns (gain results) for the monopole microstrip patch antenna on brim santista substrate. In Figure 5(a), a good agreement is observed between WCIP and HFSS software simulation results for 2D radiation pattern (gain results). It should be emphasized what this work’s contribution is in using WCIP to calculate the radiation pattern for the proposed antenna, a fact that has not been reported (as far as we are concerned) in the literature. Considering the 2D results, the antenna gain keeps almost constant for variations in the range −100° < θ < 100°. In Figure 5(b), the antenna radiation pattern (gain results) looks omnidirectional (HFSS results), a good performance for wireless system applications.Figure 5
Radiation patterns (gain results) for the monopole microstrip antenna on brim santista substrate: (a) 2D and (b) 3D results.
(a)
(b)Table1 presents resonant frequency, VSWR, and gain results for the proposed antenna. These results have been obtained by WCIP formulation, HFSS software, and measurements, for comparison purpose. These results are in good agreement and have been obtained using the lowest value of s11, for the resonant frequency fr, and the maximum VSWR value in the UWB band, and the maximum gain for −100° < θ < 100°.Table 1
Simulation and Measurements Results.
Parameter
WCIP
HFSS
Measurements
f
r (GHz)
6.51
6.63
6.67
VSWR
1.16
1.49
1.60
Gain
0.640
0.632
—Based on the results shown in Table1, the proposed antenna is a good candidate for UWB system applications. In addition, the WCIP formulation has proven to be efficient and successful in characterizing the proposed monopole microstrip patch antennas with a complex Mandelbrot fractal geometry. In addition, it can be used in the analysis of other complex planar structures, such as antennas, filters, couplers, power dividers, and FSSs, in microstrip or CPW geometries, including the analysis of printed circuits on nonconventional materials.


## 5. Conclusion

A microstrip antenna for UWB applications printed on a textile substrate has been analyzed using the WCIP method. The monopole antenna is based on a resonant patch element with Mandelbrot fractal geometry. WCIP formulation has been used in the determination of the antenna resonant frequencies, return loss, and radiation pattern (gain results). The WCIP theoretical, HFSS simulation, and measurement results indicate that the proposed antenna can operate in the whole UWB band. In addition, the monopole antenna has presented omnidirectional radiation characteristics. Finally, an excellent agreement between measured and simulated results has been observed confirming the good performance of the proposed antenna and efficiency of the used numerical analysis technique (WCIP method).



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*Source: 4686315-2017-11-07.xml*