# Design of UWB Wearable Conformal Antenna Based on Jean Material

Authors: Peng Chen; Dan Wang; Lu Liu; Lihua Wang; Yumeng Lin
Journal: International Journal of Antennas and Propagation
 (2022)

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## Abstract

In this paper, a wearable ultra-wideband (UWB) microstrip antenna is designed to meet the demand for Wireless Body Area Network (WBAN). This is a wearable textile antenna, which was formed on a jeans fabric substrate to reduce surface-wave losses. The single-fed circular strip monopole antenna provides good impedance matching over the entire UWB frequency range of 2.9∼10.6 GHz. The dielectric constantεr  = 2.2, and the loss tangent tanδ  = 0.04 of the jean substrates are measured by using the coaxial ring method. The proposed antenna consists of an improved circular radiation patch with the defective ground structure to expand the frequency band of the antenna and improve the radiation characteristics of the antenna with small dimensions of 20×30×1.4mm3. In addition, structural deformation of the proposed antenna is performed to analyze the flexibility of the proposed antenna. The simulated SAR values follow the FCC limit, making it most suitable for wearable applications.


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## Body

## 1. Introduction

WBANs are networks distributed around the human body. WBAN is mainly used to detect and transmit the user’s physiological data and cooperates with other networks to integrate the human body into the overall network [1]. Nowadays, wearable electronics are becoming popular and usability, functionality, durability, safety, and comfort have become essential elements of wearable systems [2]. The potential applications of wearable antennas for tracking, navigation, public safety, and health monitoring are also increasing [3]. In military applications, wearable antennas can provide personal positioning and mobile communication through helmets [4, 5]. In healthcare, wearable antennas can monitor physiological information, such as blood pressure, blood glucose concentration, temperature, weight, and heartbeat [6–8]. These applications face limitations due to electromagnetic coupling between the human body and the antenna, changing physical deformations, highly variable operating environments, and manufacturing processes [9–11].Wearable systems require antennas as transmitters and receivers. Bending and stretching of flexible and wearable antennas during use not only affects resonance frequency but also the radiation characteristics of the wearable antenna, especially when it requires circular polarization. Flexibility, lightweight, comfort, and robustness are essential features for designing wearable antennas [12]. Textile antennas are therefore a strong candidate for wearable applications. Textile-based antennas with easy integration with clothing and without interfering with the user; various textile materials such as flannel, felt, denim, polyester, and cotton have been used as substrates. The relative dielectric constant of the fabric material is between 1.05 and 1.9, and the loss tanσ is between 0.0001 and 0.025, which depends on the working frequency, moisture content, fabric structural properties, and bulk density of the fabric material [13]. A felt-based wearable antenna for 2.4/5.2 GHz dual-band operation in WLAN applications with a maximum gain of 1.8 dBi/3.2 dBi has been proposed in [14]. Polyester and denim textiles have been used in wearable antennas that provide a frequency range of 2.25∼2.74 GHz and 4.3∼6.8 GHz for WLAN and WiMAX band applications [15]. In comparison, the inherent flexibility and lightweight properties of denim materials can provide more convenience for users in real-time environments [16, 17]. In [18], a circular slotted textile antenna with a partially grounded structure with an impedance bandwidth of approximately 46% and 41%, respectively, has been proposed. Its results show that denim fabrics are good candidates for textile wearable applications. Denim fabric is also one of the best choices for designing UWB circular patch antennas [19, 20]. It has been observed that the antennas are designed using complex structures of radiators to cover the target frequency range [14, 21]. Wearable antennas do not have structural deformations, and human experiments analyze the changes in antenna performance [18–24]. The antenna [17, 20] results in a large antenna dimension and increases the design complexity of the receiver front-end systems. The proposed antenna overcomes the above-mentioned issues and provides novel features such as a compact, simple structure, and covers the entire UWB frequency range. The antenna sustains its performance in terms of impedance bandwidth, radiation pattern, and current distribution even when tested on body tissues suitable for on-head communication.In this paper, a wearable antenna with an improved circular patch for WBAN is proposed, which uses denim fabric as the substrate and consists of a circular radiating patch with a square slot in the middle, a rectangular microstrip line, and a defective ground structure to achieve the coverage of the whole UWB frequency range from 3.1 GHz to 10.6 GHz. A stable omnidirectional radiation pattern is obtained with the required gain and efficiency over the entire UWB frequency range. The antenna is small in size, bendable, easy to integrate, easy to process, and suitable to be integrated to wear on a hat.


## 2. Antenna Structure and Design

### 2.1. Fabric Characterization

The transmission-reflection method has the advantages of easy operation and fast measurement speed. The method can be divided into the coaxial circular method and the rectangular waveguide method according to the different measurement fixtures. The coaxial circular method has a wide range of measurements and is easy to prepare specimens; the rectangular waveguide method requires separate measurements of each waveband and is more complicated to prepare specimens. Therefore, in this paper, the coaxial circular method of transmission reflection is used to measure the dielectric constant of denim fabrics.The coaxial ring method is used to measure the electromagnetic parameters of the denim fabric, and the test sample needs to be calibrated with mechanical or automatic calibration parts before testing. After the calibration is completed, a circular sample with the same inner and outer diameter is prepared with a grinding tool and placed in the fixture. The instrument emits a wave signal of a specific frequency through one port, which is reflected in the fixture containing the sample through the transmission to respond. Then the other end of the cable is transmitted back to the instrument for analysis and calculation, and finally, the computer can directly display the electromagnetic parameters of the material. [25, 26].The dielectric constant of denim fabric isεr=ε′−jε″. The magnetic permeability of denim fabric is ur=u′−ju″. ε′, ε″ are the real and imaginary parts of the dielectric constant of the material, respectively. u′, u″ are the real and imaginary parts of the magnetic permeability of the material. Dielectric loss tangent is tanδ=ε″/ε′.This paper uses the Keysight N5222 B Vector Network Analyzer (VNA) mainly to measureε′, μ′, and μ″. A schematic diagram of electromagnetic property measuring equipment is shown in Figure 1(a). A de-embedding technique that compensates both phase and magnitude was used to get the S-parameter of the device under test (DUT), which is shown in Figure 1(b). The relative permittivity and permeability of the material as a function of frequency are given in Figure 2. Thus, the substrate used in the proposed antenna has a relative permittivity of 2.2, a permeability of 1.0, and a loss tangent of 0.04.Figure 1
Schematic diagram of electromagnetic property measuring equipment and sample: (a) equipment for coaxial ring method test; (b) DUT.Figure 2
Measured permittivity and permeability.


### 2.2. Evolution of Antenna

Different from the previous studies of UWB antennas [27–30], the ultra-wideband microstrip antenna designed in this paper is made of jean cloth as the medium substrate, a circular radiation patch with a square slot in the middle, a rectangular microstrip line, and a defective ground structure. The antenna is a circular patch antenna with an open rectangular slot in the middle, which can generate ultra-wideband operating frequency bands through its resonance characteristics. Compared with the triangular or elliptical gap ultra-wideband, the antenna has more adjustable dimensional parameters due to its defective structure, making it easier to achieve impedance matching. This type of defect plays an important role in the bandwidth and wideband characteristics of the antenna.The structure of the circular ultra-wideband antenna designed in this article is shown in Figure3. The dielectric substrate is 20×30×1.4mm3, and studies on all impedance matching have resulted in a 50 Ω microstrip feeder for antenna feed achieved by the HFSS 19.0. The key parameters of the antenna are optimized with the optimization goal of performance and impedance matching, and the specific antenna size parameters are shown in Table 1.Figure 3
Geometry of the proposed antenna. (a) Front view. (b) Rear view.Table 1
Antenna basic size parameters.
ParametersSizes (mm)ParametersSizes (mm)ParametersSizes (mm)W20L30L410W16L112L510W23.5L28R18.1A1.4L35.5R21.4As shown in Figure4, the design process of the ultra-wideband antenna structure is described in this paper. Figure 5 and Figure 6 show the s11 and surface current distribution of the antenna at different stages. Figure 4(a) depicts the original structure of the antenna design, using a 50 Ω rectangular microstrip line, a circular radiation patch, and a rectangular ground plate. The antenna model is a simple and small-size antenna. The original model’s working band is 3.5 GHz to 10 GHz and 10.3 GHz to 14.5 GHz (stage 1).Figure 4
The design process of the UWB antenna. (a) Round monopole antenna. (b) Slotted circular antenna. (c) Microstrip antenna with rectangular slot. (d) Improved circular microstrip antenna with asymmetric defect ground.Figure 5
Simulated reflection coefficient of the evolution of the antenna.Figure 6
Simulation results of the current distribution of the UWB antenna with a phase of 0: (a) stage 1, (b) stage 2, (c) stage 3, and (d) stage 4.
(a)(b)(c)(d)Rectangular slots are cut in the antenna base plate and asymmetric rectangular slots are cut in the center of the circular radiating patch at stage 2. After adding slots, the current paths have been changed by the inserted structures at 8 and 10 GHz separately. It can be observed that the current flowing through the slot becomes larger, causing a slight shift in the resonant frequency point of stage 2 compared to stage 1. The operating bandwidth of the antenna is set to be 3.4 GHz to 9.6 GHz and 11.1 GHz to 14.6 GHz.Based on structure 2, rectangular slots are added in the center of the circular radiation patch and grounding plate. The operating bandwidth of the antenna is further improved so that the return loss is less than −10 dB in the bandwidth from 3.42 GHz to 15 GHz (stage 3). However, some low-frequency parts are still not covered in the UWB (3.1∼10.6 GHz).Based on structure 3, the upper edge is detriangulated to obtain the final model of the antenna (stage 4). After the slotting, the working bandwidth of the antenna is extended to a certain degree in the low-frequency part, and the working bandwidth of the antenna is from 2.9 GHz to 15 GHz, which meets the communication requirements of the UWB. The simulated reflection coefficient characteristics of the evolution of the proposed antenna are shown in Figure5.The current distribution results bring to light the idea of understanding how the current flows in the conductive region of the simulated UWB wearable antenna. Figure7 shows these results for the proposed antenna design using denim fabric as the substrate along with copper as the conductor material. The antenna bends on a cylindrical model with a radius of 50 mm. Simulate and measure thebending in the X and Y directions and observe the results. For discussion samples at 4 GHz, 6 GHz, and 8 GHz for three different frequencies have been provided. As can be seen from Figure 8, the intensity of the current is high in the frequency range from 4 GHz to 6 GHz. The high-intensity currents at 4 GHz and 6 GHz are found to be radiated along the conductive part of the antenna, especially along the transmission line as well as in the middle of the circular patch. On the other hand, at 8 GHz, high current intensity was found at both ends of the transmission line and at the bottom of the circular patch.Figure 7
Structural deformation. (a) SimulatedX-bend. (b) Simulated Y-bend. (c) Measured X-bend. (d) Measured Y-bend.Figure 8
Simulation results of the current distribution of UWB antenna in free space for three different frequency samples: (a) 4 GHz, (b) 6 GHz, and (c) 8 GHz.
(a)(b)(c)


### 2.3. Fabrication

The antenna is based on denim fabric with copper as the conductive material. Due to the limitations of the process, copper cannot be directly attached to the fabric substrate. The adhesion of the conductive material to the fabric substrate is very important. Therefore, copper was chosen to cover the FPC flex board. In other words, the radiating patch and ground are covered on the FPC flex board, and the substrate is sandwiched between the flex boards so that the conductive material is evenly placed on the denim and fixed. It forms an antenna structure with radiant elements and FPC flexible board as the top layer, jean fabric as the substrate material, and FPC flexible board and grounding metal as the bottom layer. The specific dimensions are shown in Table2. In antenna fabrication, direct metal soldering is used to connect the top radiating patch and ground plane to the coaxial connector. Antennas are manufactured to meet the requirements of the wearer’s demands for compact size, flexible materials, easy to clean, and very attractive wearable devices.Table 2
Dimensions of the designed wearable UWB antenna.
LocationSubstrate thickness (mm)Substrate dimensions (mm)FPC thickness (mm)FPC dimensions (mm)Sizes120×300.220×30


## 2.1. Fabric Characterization

The transmission-reflection method has the advantages of easy operation and fast measurement speed. The method can be divided into the coaxial circular method and the rectangular waveguide method according to the different measurement fixtures. The coaxial circular method has a wide range of measurements and is easy to prepare specimens; the rectangular waveguide method requires separate measurements of each waveband and is more complicated to prepare specimens. Therefore, in this paper, the coaxial circular method of transmission reflection is used to measure the dielectric constant of denim fabrics.The coaxial ring method is used to measure the electromagnetic parameters of the denim fabric, and the test sample needs to be calibrated with mechanical or automatic calibration parts before testing. After the calibration is completed, a circular sample with the same inner and outer diameter is prepared with a grinding tool and placed in the fixture. The instrument emits a wave signal of a specific frequency through one port, which is reflected in the fixture containing the sample through the transmission to respond. Then the other end of the cable is transmitted back to the instrument for analysis and calculation, and finally, the computer can directly display the electromagnetic parameters of the material. [25, 26].The dielectric constant of denim fabric isεr=ε′−jε″. The magnetic permeability of denim fabric is ur=u′−ju″. ε′, ε″ are the real and imaginary parts of the dielectric constant of the material, respectively. u′, u″ are the real and imaginary parts of the magnetic permeability of the material. Dielectric loss tangent is tanδ=ε″/ε′.This paper uses the Keysight N5222 B Vector Network Analyzer (VNA) mainly to measureε′, μ′, and μ″. A schematic diagram of electromagnetic property measuring equipment is shown in Figure 1(a). A de-embedding technique that compensates both phase and magnitude was used to get the S-parameter of the device under test (DUT), which is shown in Figure 1(b). The relative permittivity and permeability of the material as a function of frequency are given in Figure 2. Thus, the substrate used in the proposed antenna has a relative permittivity of 2.2, a permeability of 1.0, and a loss tangent of 0.04.Figure 1
Schematic diagram of electromagnetic property measuring equipment and sample: (a) equipment for coaxial ring method test; (b) DUT.Figure 2
Measured permittivity and permeability.


## 2.2. Evolution of Antenna

Different from the previous studies of UWB antennas [27–30], the ultra-wideband microstrip antenna designed in this paper is made of jean cloth as the medium substrate, a circular radiation patch with a square slot in the middle, a rectangular microstrip line, and a defective ground structure. The antenna is a circular patch antenna with an open rectangular slot in the middle, which can generate ultra-wideband operating frequency bands through its resonance characteristics. Compared with the triangular or elliptical gap ultra-wideband, the antenna has more adjustable dimensional parameters due to its defective structure, making it easier to achieve impedance matching. This type of defect plays an important role in the bandwidth and wideband characteristics of the antenna.The structure of the circular ultra-wideband antenna designed in this article is shown in Figure3. The dielectric substrate is 20×30×1.4mm3, and studies on all impedance matching have resulted in a 50 Ω microstrip feeder for antenna feed achieved by the HFSS 19.0. The key parameters of the antenna are optimized with the optimization goal of performance and impedance matching, and the specific antenna size parameters are shown in Table 1.Figure 3
Geometry of the proposed antenna. (a) Front view. (b) Rear view.Table 1
Antenna basic size parameters.
ParametersSizes (mm)ParametersSizes (mm)ParametersSizes (mm)W20L30L410W16L112L510W23.5L28R18.1A1.4L35.5R21.4As shown in Figure4, the design process of the ultra-wideband antenna structure is described in this paper. Figure 5 and Figure 6 show the s11 and surface current distribution of the antenna at different stages. Figure 4(a) depicts the original structure of the antenna design, using a 50 Ω rectangular microstrip line, a circular radiation patch, and a rectangular ground plate. The antenna model is a simple and small-size antenna. The original model’s working band is 3.5 GHz to 10 GHz and 10.3 GHz to 14.5 GHz (stage 1).Figure 4
The design process of the UWB antenna. (a) Round monopole antenna. (b) Slotted circular antenna. (c) Microstrip antenna with rectangular slot. (d) Improved circular microstrip antenna with asymmetric defect ground.Figure 5
Simulated reflection coefficient of the evolution of the antenna.Figure 6
Simulation results of the current distribution of the UWB antenna with a phase of 0: (a) stage 1, (b) stage 2, (c) stage 3, and (d) stage 4.
(a)(b)(c)(d)Rectangular slots are cut in the antenna base plate and asymmetric rectangular slots are cut in the center of the circular radiating patch at stage 2. After adding slots, the current paths have been changed by the inserted structures at 8 and 10 GHz separately. It can be observed that the current flowing through the slot becomes larger, causing a slight shift in the resonant frequency point of stage 2 compared to stage 1. The operating bandwidth of the antenna is set to be 3.4 GHz to 9.6 GHz and 11.1 GHz to 14.6 GHz.Based on structure 2, rectangular slots are added in the center of the circular radiation patch and grounding plate. The operating bandwidth of the antenna is further improved so that the return loss is less than −10 dB in the bandwidth from 3.42 GHz to 15 GHz (stage 3). However, some low-frequency parts are still not covered in the UWB (3.1∼10.6 GHz).Based on structure 3, the upper edge is detriangulated to obtain the final model of the antenna (stage 4). After the slotting, the working bandwidth of the antenna is extended to a certain degree in the low-frequency part, and the working bandwidth of the antenna is from 2.9 GHz to 15 GHz, which meets the communication requirements of the UWB. The simulated reflection coefficient characteristics of the evolution of the proposed antenna are shown in Figure5.The current distribution results bring to light the idea of understanding how the current flows in the conductive region of the simulated UWB wearable antenna. Figure7 shows these results for the proposed antenna design using denim fabric as the substrate along with copper as the conductor material. The antenna bends on a cylindrical model with a radius of 50 mm. Simulate and measure thebending in the X and Y directions and observe the results. For discussion samples at 4 GHz, 6 GHz, and 8 GHz for three different frequencies have been provided. As can be seen from Figure 8, the intensity of the current is high in the frequency range from 4 GHz to 6 GHz. The high-intensity currents at 4 GHz and 6 GHz are found to be radiated along the conductive part of the antenna, especially along the transmission line as well as in the middle of the circular patch. On the other hand, at 8 GHz, high current intensity was found at both ends of the transmission line and at the bottom of the circular patch.Figure 7
Structural deformation. (a) SimulatedX-bend. (b) Simulated Y-bend. (c) Measured X-bend. (d) Measured Y-bend.Figure 8
Simulation results of the current distribution of UWB antenna in free space for three different frequency samples: (a) 4 GHz, (b) 6 GHz, and (c) 8 GHz.
(a)(b)(c)


## 2.3. Fabrication

The antenna is based on denim fabric with copper as the conductive material. Due to the limitations of the process, copper cannot be directly attached to the fabric substrate. The adhesion of the conductive material to the fabric substrate is very important. Therefore, copper was chosen to cover the FPC flex board. In other words, the radiating patch and ground are covered on the FPC flex board, and the substrate is sandwiched between the flex boards so that the conductive material is evenly placed on the denim and fixed. It forms an antenna structure with radiant elements and FPC flexible board as the top layer, jean fabric as the substrate material, and FPC flexible board and grounding metal as the bottom layer. The specific dimensions are shown in Table2. In antenna fabrication, direct metal soldering is used to connect the top radiating patch and ground plane to the coaxial connector. Antennas are manufactured to meet the requirements of the wearer’s demands for compact size, flexible materials, easy to clean, and very attractive wearable devices.Table 2
Dimensions of the designed wearable UWB antenna.
LocationSubstrate thickness (mm)Substrate dimensions (mm)FPC thickness (mm)FPC dimensions (mm)Sizes120×300.220×30


## 3. Results and Discussion

The performance of the antenna is analyzed by using parameters such as reflection coefficient, radiation pattern, gain, and efficiency. The fabricated prototype of the proposed antenna is shown in Figure9. The simulation is performed using the HFSS 19.0 and measurements are carried out using Keysight’s 3672D Vector Network Analyzer.Figure 9
(a) Fabricated textile antenna front and back view. (b) Vector network analyzer. (c) Radiation pattern measured in free space.


### 3.1. Measurement and Simulation Results

The effect on the antenna performance can be evaluated with the human brain model of the human body structure that comes with HFSS. However, the human brain model has a very dense mesh with distinct contour features and a long simulation time. To simplify the study environment, a spherical container and brain tissue fluid are used to simulate a simple human head model. The relative permittivity of the brain tissue fluid is 41.5 with a loss tangent of 0.90, and the relative permittivity of the shell is 4.6 with a loss angle tangent of 0.01.As shown in Figure10, the simple human head model has a hollow spherical shell with a radius of 111.5 mm and a thickness of 5 mm. The brain tissue fluid is a spherical model with a radius of 106.5 mm. The results were observed by placing the antenna on the head of a human volunteer with a height and weight of 155 cm(45 kg) for measurement. Considering that the antenna is wearable, the distance between the antenna and the manikin is kept at 10 mm.Figure 10
The simulation model of the human brain.The simulation of the proposed antenna provides a frequency range from 2.9 GHz to 15 GHz. The anthropometric results provide a frequency range of 2.8 GHz to 10.8 GHz. Figure11 shows a comparison of the characteristics of the simulated and measured reflection coefficients in free space and in the human body. However, free space and physical outcomes are interrelated, and even though the actual bandwidth of the antenna becomes smaller, it still covers the entire ultra-wideband frequency range. The slight change between simulated and measured results is due to the flexibility of the textile material, fabrication tolerance, humidity, and temperature effect on cotton. However, simulated and measured results show a good correlation.Figure 11
Simulates and measures the reflective coefficient of the proposed antenna in free space and on the human body.The radiation patterns are measured in the anechoic chamber. Figure12 depicts a comparison of the simulated and measured normalized directional maps of the proposed antenna in the YOZ-plane and XOZ-plane of the free space at different frequencies, such as 4 GHz, 6.5 GHz, and 8 GHz. A stable radiation pattern is observed over the entire frequency range. It can be observed from the figure that the proposed antenna has omnidirectional radiation in the XOZ-plane.Figure 12
Free space comparison of simulated and measurement radiation pattern in the YOZ-plane and XOZ-plane. (a) 4 GHz. (b) 6.5 GHz. (c) 8 GHz.
(a)(b)(c)


### 3.2. Structural Deformation

It is difficult to keep the antenna flat at all times in wearable systems, especially when the antenna is made of textile materials. Since the designed antenna is integrated into a cowboy hat, it is necessary to study the performance characteristics of the antenna under bending conditions. When the antenna is placed on the human body, the antenna performance will be strongly affected due to the electromagnetic coupling and specific absorption of the human body. The high dielectric constant and conductivity of human tissue affect the performance and propagation loss of the antenna. Therefore, the analysis of the structural deformation is necessary to better understand the flexible characteristics of the antenna.Figure13 provides a comparison of the simulated and measured reflection coefficient characteristics due to structural deformation with the conditions of bending in the y-direction on the human body model. From the figure, it can be concluded that the proposed antenna has a slight shift in the resonance point in the Y-direction bending towards the high frequency. It still covers the entire UWB (3.1 to 10.6 GHz), compared to the results obtained on the planar model. In the simulations and measurements under flat conditions, the measured antenna covers the frequency range from 2.9 GHz to 10.6 GHz with better impedance matching compared to the simulated results. Even though the proposed antenna is slightly shifted in the Y-direction bending the human head experiment, it provides an acceptable band coverage from 3.1 GHz to 10.2 GHz.Figure 13
Comparison of the characteristics of the simulation and measurement of reflection coefficients caused by structural deformation on the human head.Figure14 provides the normalized radiation patterns of the YOZ-plane and XOZ-plane due to structural deformation simulated on the human body. The radiation patterns obtained under the X-directional bending condition show slight deviations, but they still provide the required XOZ-plane omnidirectional radiation pattern for human body communication at different frequencies such as 4 GHz, 6 GHz, and 8 GHz. Therefore, the gain and efficiency obtained for the proposed antenna under the structural deformation with bending in the X-direction are small compared to the results for the free space variation as shown in Table 3. The proposed antenna still maintains its characteristics in terms of impedance bandwidth, radiation pattern, gain, and efficiency under structural deformation in the WBAN application situation.Figure 14
Comparison of simulated radiation patterns on the human head due to deformation of different structures in the YOZ-plane and XOZ-plane. (a) 4 GHz. (b) 6 GHz. (c) 8 GHz.Table 3
Simulated gain and radiation efficiency of the antenna after structural deformation.
Frequency (GHz)Flat positionX-orientationY-orientationGain (dB)Efficiency (%)Gain (dB)Efficiency (%)Gain (dB)Efficiency (%)31.5192.51.0491.71.0892.641.8491.91.5691.851.6192.251.9288.12.1787.71.9588.462.1688.22.387.52.3388.372.6490.52.786.22.7888.382.6888.03.0282.83.0385.492.6284.93.1282.63.0285.6103.0383.72.8781.92.7085.3112.8279.32.4478.32.8085.2


### 3.3. Analysis of Specific Absorption Rate

Electromagnetic waves emitted by antennas cause radiation to penetrate the human body. SAR is the electromagnetic power absorbed or consumed by a unit mass of human tissue in W/kg. Different national organizations have different SAR limit standards. These standards recommend safe levels of radio radiation for the public as well as for workers. The SAR limits set by the FCC are 1.6 W/kg for 1 Gram of tissue and 2 W/kg for 10 grams of tissue. Wearable antennas must meet the safety limits. The distance between the antenna and the human head model is maintained at 10 mm. Figure15 illustrates the 3D SAR distribution of the proposed antenna at 4 GHz, 6 GHz, and 8 GHz resonance frequencies in the head position with the maximum SAR values of 1.86 W/kg, 1.74 W/kg, and 1.52 W/kg for 10 g of tissue, respectively. Thus, the proposed antenna provides a limited SAR value that makes it most suitable for real-time applications.Figure 15
SAR analysis. (a) 4 GHz. (b) 6 GHz. (c) 8 GHz.
(a)(b)(c)After investigating and evaluating the proposed antenna’s performance under various conditions, it can be concluded that the proposed antenna is a reliable candidate as a wearable device for the WBAN.Table4 illustrates the close comparison of the proposed work with some recent similar works. It shows that the proposed antenna achieved a wider BW and higher radiation efficiency. The proposed antenna obtained these outcomes with smaller dimensions (it should be mentioned that the width of an antenna plays a direct impact on its efficiency and BW: when an antenna has larger dimensions, both gain and efficiency increase [33]).Table 4
Comparison with existing literature.
Ref no.Sizes (mm)RadiatorBW (GHz)SubstrateMax radiation efficiency (%)Max gain (dBi)[22]25×30Modified octagonal strip monopole antenna3.1–10.6Jeans824.4[21]88×97Fully textile microstrip topology3–10Felt627.75[18]40×40Octagonal slot-loaded circular-shaped textile antenna3.01–5.30 8.12–12.35Jeans945.7[31]67×80Two modified arc-shaped patches antenna3.7–10.3PDMS455[20]60×60Fully textile materials antenna3–20Flannel977.4[32]70×70Aperture-stacked patch antenna3–6Rogers48-[33]50×60Full ground UWB antenna7–28Jeans9610.5[34]56×70Rectangular radiating patch antenna3.6–11.3Jeans-3.57Proposed20×30Modified circular radiating patch antenna2.9–10.6Jeans92.63.12


## 3.1. Measurement and Simulation Results

The effect on the antenna performance can be evaluated with the human brain model of the human body structure that comes with HFSS. However, the human brain model has a very dense mesh with distinct contour features and a long simulation time. To simplify the study environment, a spherical container and brain tissue fluid are used to simulate a simple human head model. The relative permittivity of the brain tissue fluid is 41.5 with a loss tangent of 0.90, and the relative permittivity of the shell is 4.6 with a loss angle tangent of 0.01.As shown in Figure10, the simple human head model has a hollow spherical shell with a radius of 111.5 mm and a thickness of 5 mm. The brain tissue fluid is a spherical model with a radius of 106.5 mm. The results were observed by placing the antenna on the head of a human volunteer with a height and weight of 155 cm(45 kg) for measurement. Considering that the antenna is wearable, the distance between the antenna and the manikin is kept at 10 mm.Figure 10
The simulation model of the human brain.The simulation of the proposed antenna provides a frequency range from 2.9 GHz to 15 GHz. The anthropometric results provide a frequency range of 2.8 GHz to 10.8 GHz. Figure11 shows a comparison of the characteristics of the simulated and measured reflection coefficients in free space and in the human body. However, free space and physical outcomes are interrelated, and even though the actual bandwidth of the antenna becomes smaller, it still covers the entire ultra-wideband frequency range. The slight change between simulated and measured results is due to the flexibility of the textile material, fabrication tolerance, humidity, and temperature effect on cotton. However, simulated and measured results show a good correlation.Figure 11
Simulates and measures the reflective coefficient of the proposed antenna in free space and on the human body.The radiation patterns are measured in the anechoic chamber. Figure12 depicts a comparison of the simulated and measured normalized directional maps of the proposed antenna in the YOZ-plane and XOZ-plane of the free space at different frequencies, such as 4 GHz, 6.5 GHz, and 8 GHz. A stable radiation pattern is observed over the entire frequency range. It can be observed from the figure that the proposed antenna has omnidirectional radiation in the XOZ-plane.Figure 12
Free space comparison of simulated and measurement radiation pattern in the YOZ-plane and XOZ-plane. (a) 4 GHz. (b) 6.5 GHz. (c) 8 GHz.
(a)(b)(c)


## 3.2. Structural Deformation

It is difficult to keep the antenna flat at all times in wearable systems, especially when the antenna is made of textile materials. Since the designed antenna is integrated into a cowboy hat, it is necessary to study the performance characteristics of the antenna under bending conditions. When the antenna is placed on the human body, the antenna performance will be strongly affected due to the electromagnetic coupling and specific absorption of the human body. The high dielectric constant and conductivity of human tissue affect the performance and propagation loss of the antenna. Therefore, the analysis of the structural deformation is necessary to better understand the flexible characteristics of the antenna.Figure13 provides a comparison of the simulated and measured reflection coefficient characteristics due to structural deformation with the conditions of bending in the y-direction on the human body model. From the figure, it can be concluded that the proposed antenna has a slight shift in the resonance point in the Y-direction bending towards the high frequency. It still covers the entire UWB (3.1 to 10.6 GHz), compared to the results obtained on the planar model. In the simulations and measurements under flat conditions, the measured antenna covers the frequency range from 2.9 GHz to 10.6 GHz with better impedance matching compared to the simulated results. Even though the proposed antenna is slightly shifted in the Y-direction bending the human head experiment, it provides an acceptable band coverage from 3.1 GHz to 10.2 GHz.Figure 13
Comparison of the characteristics of the simulation and measurement of reflection coefficients caused by structural deformation on the human head.Figure14 provides the normalized radiation patterns of the YOZ-plane and XOZ-plane due to structural deformation simulated on the human body. The radiation patterns obtained under the X-directional bending condition show slight deviations, but they still provide the required XOZ-plane omnidirectional radiation pattern for human body communication at different frequencies such as 4 GHz, 6 GHz, and 8 GHz. Therefore, the gain and efficiency obtained for the proposed antenna under the structural deformation with bending in the X-direction are small compared to the results for the free space variation as shown in Table 3. The proposed antenna still maintains its characteristics in terms of impedance bandwidth, radiation pattern, gain, and efficiency under structural deformation in the WBAN application situation.Figure 14
Comparison of simulated radiation patterns on the human head due to deformation of different structures in the YOZ-plane and XOZ-plane. (a) 4 GHz. (b) 6 GHz. (c) 8 GHz.Table 3
Simulated gain and radiation efficiency of the antenna after structural deformation.
Frequency (GHz)Flat positionX-orientationY-orientationGain (dB)Efficiency (%)Gain (dB)Efficiency (%)Gain (dB)Efficiency (%)31.5192.51.0491.71.0892.641.8491.91.5691.851.6192.251.9288.12.1787.71.9588.462.1688.22.387.52.3388.372.6490.52.786.22.7888.382.6888.03.0282.83.0385.492.6284.93.1282.63.0285.6103.0383.72.8781.92.7085.3112.8279.32.4478.32.8085.2


## 3.3. Analysis of Specific Absorption Rate

Electromagnetic waves emitted by antennas cause radiation to penetrate the human body. SAR is the electromagnetic power absorbed or consumed by a unit mass of human tissue in W/kg. Different national organizations have different SAR limit standards. These standards recommend safe levels of radio radiation for the public as well as for workers. The SAR limits set by the FCC are 1.6 W/kg for 1 Gram of tissue and 2 W/kg for 10 grams of tissue. Wearable antennas must meet the safety limits. The distance between the antenna and the human head model is maintained at 10 mm. Figure15 illustrates the 3D SAR distribution of the proposed antenna at 4 GHz, 6 GHz, and 8 GHz resonance frequencies in the head position with the maximum SAR values of 1.86 W/kg, 1.74 W/kg, and 1.52 W/kg for 10 g of tissue, respectively. Thus, the proposed antenna provides a limited SAR value that makes it most suitable for real-time applications.Figure 15
SAR analysis. (a) 4 GHz. (b) 6 GHz. (c) 8 GHz.
(a)(b)(c)After investigating and evaluating the proposed antenna’s performance under various conditions, it can be concluded that the proposed antenna is a reliable candidate as a wearable device for the WBAN.Table4 illustrates the close comparison of the proposed work with some recent similar works. It shows that the proposed antenna achieved a wider BW and higher radiation efficiency. The proposed antenna obtained these outcomes with smaller dimensions (it should be mentioned that the width of an antenna plays a direct impact on its efficiency and BW: when an antenna has larger dimensions, both gain and efficiency increase [33]).Table 4
Comparison with existing literature.
Ref no.Sizes (mm)RadiatorBW (GHz)SubstrateMax radiation efficiency (%)Max gain (dBi)[22]25×30Modified octagonal strip monopole antenna3.1–10.6Jeans824.4[21]88×97Fully textile microstrip topology3–10Felt627.75[18]40×40Octagonal slot-loaded circular-shaped textile antenna3.01–5.30 8.12–12.35Jeans945.7[31]67×80Two modified arc-shaped patches antenna3.7–10.3PDMS455[20]60×60Fully textile materials antenna3–20Flannel977.4[32]70×70Aperture-stacked patch antenna3–6Rogers48-[33]50×60Full ground UWB antenna7–28Jeans9610.5[34]56×70Rectangular radiating patch antenna3.6–11.3Jeans-3.57Proposed20×30Modified circular radiating patch antenna2.9–10.6Jeans92.63.12


## 4. Conclusions

An ultra-wideband wearable conformal antenna based on jean fabric is designed. The antenna satisfies the WBAN requirements and uses denim fabric as the substrate, which can be integrated into a hat. The proposed antenna provides good impedance matching throughout the UWB frequency range through a circular radiating patch with a rectangular slot in the middle, a rectangular microstrip line, and a defective ground structure. While examining the performance of the antenna under bending and on the head, a slight shift in resonant frequency is observed. The antenna has the features of small size, easy integration, bendability, and low impact on antenna performance when placed in front of a human head, which makes it a wearable antenna with use-value. For the proposed structure, the SAR obtained is 1.86 W/Kg below the recommended value, and the SAR value should be reduced further.



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*Source: 4886844-2022-08-23.xml*