# X-Shaped Slotted Patch Biomedical Implantable Antenna for Wireless Communication Networks

Authors: Sarosh Ahmad; Bilal Manzoor; Salman Naseer; Nilton Santos-Valdivia; Adnan Ghaffar; Muhammad Inam Abbasi
Journal: Wireless Communications and Mobile Computing
 (2022)

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## Abstract

Biomedical implantable antennas have a major role in biomedical telemetry applications. Therefore, a compact-size low-profile implantable antenna working in industrial, scientific, and medical (ISM) band at 915 MHz is presented. The presented antenna is a simple slotted patch fed with a coaxial probe of 50Ω impedance. The patch consists of four slotted resonators printed on a flexible Roger Duroid RT5880 substrate (εr=2.2, tanδ=0.0009) with the standard thickness of 0.254 mm. The complete volume of the designed antenna is 7mm×7mm×0.254mm (0.08λg×0.08λg×0.003λg). The antenna covers the bandwidth from 800 MHz to 1 GHz (200 MHz) inside skin tissue. A good agreement between the simulation and measurements of the antenna has been obtained. Finally, the specific absorption rate (SAR) values have also been analyzed through simulations as 8.17 W/kg inside skin over 1 g of mass tissue. The proposed SAR values are less than the limit of the Federal Communications Commission (FCC). This antenna is miniaturized and an ideal applicant for applications in biomedical implants.


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## Body

## 1. Introduction

Implantable medical devices (IMDs) are playing a significant role in enhancing the living conditions of the patients day by day. The telemetry system has given us many advantages by using an implantable antenna for the wireless communications between IMDs and external monitoring devices, and those advantages can be in terms of high data rates and long-distance communications [1, 2]. The schematic diagram of the implantable medical devices (IMDs) is presented in Figure 1. For the proposed model of the antenna, implantable medical devices (IMDs) are the key components [3]. The in-body antenna must be very thin in profile and should have very less values of SAR, and antennas should have flexibility for human care purposes [4]. Therefore, during the design stage, the antenna must be compatible and flexible along with the human body. Human body tissues can interfere with the operating frequency which can damage the tissues; that is why the antenna should have broader bandwidth that can cover the required frequency band after being tested on human tissues [5]. The radiation properties of the antenna change rapidly due to the multiple layer structure of the human body. The human structure has skin, fat, bone, muscle, and blood tissues. These tissues have different dielectric properties which make it difficult for designing a biocompatible antenna to be utilized for the human body applications [6]. Many in-body antennas are designed for wireless communication at midradio band ranges between 402 and 405 MHz [7–11] and at ISM band ranges between 2.4 and 2.48 GHz [12–17]. A compact-sized broadband antenna for the implementations in biomedical implants operating at the MICS band (403 MHz) was presented in [8]. A semiflexible Roger 6010 substrate material was used with the thickness of 1.27 mm. SAR values were calculated as 284.5 W/kg over 1 g that is very high than our proposed design. Another ISM band biomedical antenna for implantable applications based on the polyimide substrate was reported in [10].Figure 1
Schematic diagram of the implantable medical devices (IMDs).The antenna had a realized gain of -16.8 dB and the operational bandwidth of 1.22%. The complete area of the antenna was25×20mm2. The realized gain and the operating bandwidth were reported as -34.9 dB and 14.9% over the reported frequency. A small-size in-body circularly polarized antenna with improved impedance matching for medical utilizations was presented in [18]. The radiating patch has circular shape, and there was an X-shaped slot inside the ground plane. The material used for the substrate was Rogers 3010 with a substrate height of 0.634 mm. Because of the two-layered substrate, the antenna profile is thick. But the antenna was less biocompatible to the human body and has high specific absorption rate (SAR) value of about 649 W/kg which is greater than the standard limit of IEEE/IEC 6270-1 standard over 1 g of mass tissue. Another implantable antenna at 915 MHz for wireless power transfer is reported in [19]. The complete size of the antenna was 11×11×1.27mm3, printed on a Roger 3010 substrate with an impedance bandwidth of 3.8% and the realized gain of about -29 dB. But the SAR values were not calculated, and the size of the antenna was still large with less bandwidth. An ISM band antenna for the devices in biomedical applications was reported in [20]. The antenna’s size was 15×15×1.27mm3, printed on a Roger 3010 substrate and operating at 915 MHz with the operation bandwidth of 10.6%. The antenna was being tested inside the skin, and its SAR values were found to be 517 W/kg which is a very large value than our proposed design, while another wideband implantable antenna for medical applications at the frequency of 915 MHz was proposed in [21]. The overall size of the antenna was 3.14×22.09×1.27mm3, and the substrate material used was Roger 3010 with a thickness of 1.27 mm. The impedance bandwidth was reported as 12.2%, and the realized gain was -32.8 dB at 915 MHz. The SAR values were calculated as 778 W/kg. The antenna had large size and large SAR value as compared to our proposed design.This article describes a compact-size implantable antenna for the biomedical applications operating in the ISM band at 915 MHz, sized at7×7×0.254mm3 (0.08λg×0.08λg×0.003λg). The design employs a Rogers RT5880 substrate (εr=2.2, tanδ=0.0009). At 915 MHz, the antenna’s radiation has an omnidirectional radiation pattern both in the E- and H-plane. The proposed design is configured with the full ground plane with four slotted resonators, so that it can provide wider bandwidth and reduced antenna back-radiation towards human skin tissue. For instance, the area of the skin is kept 20×20mm2. Because of the novel modified patch, the proposed antenna covers the more bandwidth at 915 MHz, and the peak gain of the antenna is comparable with the previous research. Fundamentally, the efficiency and designed antenna’s performance under the influence of the physical body are improved, and SAR values are significantly reduced. The antenna has achieved very less SAR values and more good agreement results between simulations and measurements. This paper comprises five sections. Section 1 introduces the research work. It covers the background of the proposed research, the statement of the problem, the objectives, and the significance of the research. Section 2 covers the design analysis of the proposed antenna. Section 3 highlights the fabrication and measurement result and describes the antenna testing inside the skin, and Section 4 describes the conclusion.


## 2. Proposed Antenna Design Analysis

A slotted compact-size patch antenna with a novel-shaped radiator is fed with a coaxial probe. The presented antenna contains distinct layers such as a full ground plane, a low-profile 0.254 mm thick Roger RT5880 substrate (εr=2.2 and tanδ=0.0009), and a slotted patch, as shown in Figure 2. The complete volume of the antenna is 7×7×0.254mm3 (0.08λg×0.08λg×0.003λg). The reported antenna is simulated in high-frequency structure simulator (HFSS) software, and the S11 of the antenna is found to be -25 dB at the working frequency of 915 MHz and the operating bandwidth of the designed antenna seems to be 21.85%. The optimized values of this antenna are summarized in Table 1.Figure 2
The proposed low-profile antenna with dimensions: (a) front view, (b) back view, and (c) exploded view.Table 1
List of the parameters of the proposed antenna.
ParametersValues (mm)ParametersValues (mm)L17S13.94L22.79S23.34L30.7S31.9L44.8S40.7W17S53.4W23S61.4W30.7S70.5W42.7S83.5


### 2.1. Proposed Antenna Design Procedure

The design procedure of the proposed implantable antenna is explained as follows:(1)
In step I (Figure3(a)), a triangular-shaped slot is introduced on the left side of the patch to generate a frequency band at 1.5 GHz, but return loss is not less than -10 dB as can be seen in Figure 4(2)
Then, in step II (Figure3(b)), in order to keep the value of the S11 (dB) less than -10 dB and to shift the frequency band towards a lower band, a T-shaped slot is introduced in a truncated patch to operate the antenna at 1.4 GHz(3)
Then, in step III (Figure3(b)), an X-shaped slot is introduced inside the patch. By introducing this slot, it has shifted the band from 1.4 GHz to 0.7 GHz (700 MHz)(4)
Then, in step IV (Figure3(c)), the proposed novel shape is designed to help to resonate the antenna at the desired frequency at 0.915 GHz(5)
Figure5 indicates the diagrammatic flow of the proposed antenna to show the entire work procedureFigure 3
Implantable antenna design procedure: (a) truncated patch (step I), (b) slotted truncated patch (step II), (c) X-shaped slotted patch (step III), and (d) proposed design (step IV).Figure 4
Simulation result comparison of theS11 for the design steps shown in Figure 3.Figure 5
Design and optimization procedure of the proposed antenna.


### 2.2. Parametric Analysis of the Proposed Antenna

The analysis of parameters of the implantable antenna is well explained in this section. The reflection coefficient at 0.915 GHz can be adjusted by varying the values of the important parameters such as length of the patch resonator “S2,” width of the feed patch “S4,” length of the patch slot at 45° angle “S3,” length of the upper left resonator of the patch “S8,” and changing the position of the via as presented in Figure 6. Figure 6(a) illustrates that by selecting the range of value of “S2” from 2.5 mm to 3.34 mm, the frequency band shifted from 1.6 GHz to 0.915 GHz (685 MHz). When the value of the “S4” is changed from 0.3 mm to 0.7 mm, then the frequency band shifted from 1.5 GHz to 0.915 GHz (585 MHz) as presented in Figure 6(b). From Figure 6(c), it is also noticed that when the values of the “S3” are varied from 1.6 mm to 1.8 mm, then the frequency band increases from 0.60 GHz to 0.75 GHz (150 MHz). Again, when the value of “S8” is varied from 2 mm to 3 mm, then there is a shift in the frequency from 1.7 GHz to 0.9 GHz (800 MHz) as shown in Figure 6(d). By changing the position of the via in the proposed patch antenna, the frequency band shifted higher to our targeted frequency band. It is noticed from Figure 6(e) that when the via is placed at position 1, then the frequency band was 1.4 GHz, and we got the 0.8 GHz band by changing the via from position 1 to position 2, and finally we achieved our desired frequency band 0.915 GHz by changing the via from position 2 to position 3.Figure 6
Parametric study of the antenna: (a) variation in “S2”; (b) variation in “S4”; (c) variation in “S3”; (d) variation in “S8”; (e) changing the position of the via.
(a)(b)(c)(d)(e)


### 2.3. Equivalent Circuit Modeling

An equivalent circuit model for the proposed implantable antenna is designed using Advanced Design System (ADS) software. Figure7(a) indicates the circuit model and the impedance matching Smith chart for the proposed antenna system. The circuit model consists of one capacitor, a resistor, and an inductor. Figure 7(b) presents the comparison between the reflection coefficient obtained from the proposed antenna and the proposed circuit model.Figure 7
(a) Circuit modeling and the impedance matching Smith chart. (b) Comparison of theS11 of the proposed antenna and the equivalent circuit model.
(a)(b)


## 2.1. Proposed Antenna Design Procedure

The design procedure of the proposed implantable antenna is explained as follows:(1)
In step I (Figure3(a)), a triangular-shaped slot is introduced on the left side of the patch to generate a frequency band at 1.5 GHz, but return loss is not less than -10 dB as can be seen in Figure 4(2)
Then, in step II (Figure3(b)), in order to keep the value of the S11 (dB) less than -10 dB and to shift the frequency band towards a lower band, a T-shaped slot is introduced in a truncated patch to operate the antenna at 1.4 GHz(3)
Then, in step III (Figure3(b)), an X-shaped slot is introduced inside the patch. By introducing this slot, it has shifted the band from 1.4 GHz to 0.7 GHz (700 MHz)(4)
Then, in step IV (Figure3(c)), the proposed novel shape is designed to help to resonate the antenna at the desired frequency at 0.915 GHz(5)
Figure5 indicates the diagrammatic flow of the proposed antenna to show the entire work procedureFigure 3
Implantable antenna design procedure: (a) truncated patch (step I), (b) slotted truncated patch (step II), (c) X-shaped slotted patch (step III), and (d) proposed design (step IV).Figure 4
Simulation result comparison of theS11 for the design steps shown in Figure 3.Figure 5
Design and optimization procedure of the proposed antenna.


## 2.2. Parametric Analysis of the Proposed Antenna

The analysis of parameters of the implantable antenna is well explained in this section. The reflection coefficient at 0.915 GHz can be adjusted by varying the values of the important parameters such as length of the patch resonator “S2,” width of the feed patch “S4,” length of the patch slot at 45° angle “S3,” length of the upper left resonator of the patch “S8,” and changing the position of the via as presented in Figure 6. Figure 6(a) illustrates that by selecting the range of value of “S2” from 2.5 mm to 3.34 mm, the frequency band shifted from 1.6 GHz to 0.915 GHz (685 MHz). When the value of the “S4” is changed from 0.3 mm to 0.7 mm, then the frequency band shifted from 1.5 GHz to 0.915 GHz (585 MHz) as presented in Figure 6(b). From Figure 6(c), it is also noticed that when the values of the “S3” are varied from 1.6 mm to 1.8 mm, then the frequency band increases from 0.60 GHz to 0.75 GHz (150 MHz). Again, when the value of “S8” is varied from 2 mm to 3 mm, then there is a shift in the frequency from 1.7 GHz to 0.9 GHz (800 MHz) as shown in Figure 6(d). By changing the position of the via in the proposed patch antenna, the frequency band shifted higher to our targeted frequency band. It is noticed from Figure 6(e) that when the via is placed at position 1, then the frequency band was 1.4 GHz, and we got the 0.8 GHz band by changing the via from position 1 to position 2, and finally we achieved our desired frequency band 0.915 GHz by changing the via from position 2 to position 3.Figure 6
Parametric study of the antenna: (a) variation in “S2”; (b) variation in “S4”; (c) variation in “S3”; (d) variation in “S8”; (e) changing the position of the via.
(a)(b)(c)(d)(e)


## 2.3. Equivalent Circuit Modeling

An equivalent circuit model for the proposed implantable antenna is designed using Advanced Design System (ADS) software. Figure7(a) indicates the circuit model and the impedance matching Smith chart for the proposed antenna system. The circuit model consists of one capacitor, a resistor, and an inductor. Figure 7(b) presents the comparison between the reflection coefficient obtained from the proposed antenna and the proposed circuit model.Figure 7
(a) Circuit modeling and the impedance matching Smith chart. (b) Comparison of theS11 of the proposed antenna and the equivalent circuit model.
(a)(b)


## 3. Results and Discussion

### 3.1. Antenna in Free Space

The designed biomedical implantable patch antenna is fabricated on a Roger RT5880 substrate with thickness of 0.254 mm and tested inside free space. A vector network analyzer (VNA) is used to measure theS11 of the implantable antenna. In the case of the simulated results, the designed antenna covers the bandwidths from 800 MHz to 1000 MHz (200 MHz) at 915 MHz while in the case of the measurements, the antenna covers the bandwidth from 795 MHz to 998 MHz (203 MHz) at 915 MHz as can be seen in Figure 8.Figure 8
(a) Measurement setup inside chamber. (b) Comparison of the simulation and measurement reflection coefficients (dB) of the patch antenna in free space.
(a)(b)TheE- and H-planes of the antenna are simulated and measured in free space (see Figure 9). The two-dimensional (2D) radiation pattern describes the behavior of the antenna. The designed antenna behaves as an omnidirectional pattern in both planes at the 915 MHz frequency band. The current density of the implantable antenna is shown in Figure 10. The current mainly flows around the upper- and bottom-sided resonators and feed patch. The red colored arrows indicate that the portion of the antenna has major contribution in operating at the desired frequency band.Figure 9
2D radiation pattern of the antenna in free space at 915 MHz.
(a)(b)Figure 10
Current distribution throughout the patch at 915 MHz.


### 3.2. Antenna inside the Skin

To explore the appropriateness of the antenna inside the skin for biomedical telemetry applications, the proposed design is simulated and tested inside skin tissue in this section. Consequently, to design an antenna for the applications in biotelemetry that had high precision, the presence of the human body phantoms must be taken into consideration while calculating SAR. For that, the antenna performance in proximity of human phantoms and the SAR values at 915 MHz are also evaluated. The area of the phantom box is20×20mm2 as can be seen in Figure 11. HFSS Studio is used for simulating the proposed antenna.Figure 11
Perspective view of the skin phantom box.In an ideal case, in-body antennas should be planned to avoid the significant coupling effects from the human tissues. While testing the antenna inside the skin of the human body, it is placed 2 mm deep inside the skin tissue as shown in Figure12. To estimate these effects, the reported design is kept inside a 40mm×40mm box of skin tissue. A “skin-mimicking gel” with relative permittivity (εr) of 43 and electrical conductivity (σ) of 1.40 is used, as its properties are very close to those of human skin tissue.Figure 12
Antenna inside the skin of human tissues: (a) perspective view, (b) fabricated prototype of the antenna, and (c) experimental setup to measure the pattern andS11.
(a)(b)(c)The contrast between the simulated and measuredS11 of the antenna inside the skin is described in Figure 13. The simulated S11 inside the skin indicates that the biomedical antenna operates from 780 MHz to 1000 MHz (220 MHz) at 915 MHz while the fabricated antenna inside the mimicking gel, on the other side, featured bandwidths from 785 MHz to 998 MHz (213 MHz). This proves that both simulated and measured results have good agreement among each other.Figure 13
Comparison between the simulated and measuredS11 of the antenna inside skin tissue.Figure14 presents the E- and H-planes of the simulation and measurement results of the radiation pattern inside skin tissue. The 2D radiation pattern describes the behavior of the antenna inside the skin. These far field results prove that the antenna inside the skin has an omnidirectional radiation pattern in both planes at the 915 MHz frequency band. The simulated realized gain value inside the skin is found to be -22 dB at 915 MHz, whereas measurement results give the realized gain of -28 dB at 915 MHz. The simulated and measured efficiency and gain graph is presented in Figure 15. The presented graph indicates that the antenna has simulated efficiency of 2.2% while the measured efficiency is 2.1% inside the skin.Figure 14
Simulated and measured far field results at 915 MHz inside skin tissue.
(a)(b)Figure 15
Simulated and measured gain and efficiency graph inside the skin.


### 3.3. Specific Absorption Rate (SAR)

The radiations of electromagnetic waves may cause health risks to the human body, and such risks are calculated in terms of SAR. The relationship between the input power and the SAR is as follows [10]:
(1)SAR=σ∣E2∣ρ,where σ and ρ denote the thermal conductivity (S/m) and the mass density (kg/m3), respectively, while E is the electric field intensity (V/m). The electric power intensity is related to the signal power as follows [13]:
(2)PowerWm2=EV/m2377.SAR simulations were accomplished when the proposed antenna is kept inside the skin as well as inside the muscle. Input power pin is kept constant at 0.5 W with the SAR evaluated based on the IEEE/IEC 6270-1 standard, averaged over 1 g of mass tissue. SAR values inside the skin are calculated as 8.17 W/kg at 915 MHz as presented in Figure16.Figure 16
SAR distribution of the proposed antenna inside skin tissue over 1 g at 915 MHz.


### 3.4. Link Budget Analysis

The telemetry range between the implanted device and the external base station must be determined in order to successfully communicate biological data. However, the link budget estimates are affected by a variety of losses, including free space losses, cable losses, and antenna material and mismatch losses [14]. The link margins were calculated using the Friis equation to calculate the difference between the antenna power (AP) and the necessary antenna power (RP), and the link margin should be more than 20 dB for consistent communication. Table 2 lists the important parameters utilized in these computations. The following formula can be used to calculate RP:
(3)RP=EbNo+KT+Br.Table 2
Parameters of the link budget of the stated design.
ParametersVariablesValueResonance frequencyfoMHz915Noise power densityNodB/Hz-203.93Transmitter powerPTxdBm-4Polarization mismatch lossPLdB1TemperatureToKelvin273Free space path lossLfdBDistance dependentTransmitter antenna gainGTxdBiScenario dependentReceiver antenna gainGRxdBi2Boltzmann constantK1.38×10−23Available powerAPdbDistance dependentBit rateBrMbps1Required powerRPdB-134.64The phase shift keying, Boltzmann’s constant, temperature, and bit rate are represented byEb/No, K, To, and Br, respectively. AP, on the other hand, may be computed as follows:
(4)APdB=Pa+Ga+Gb+Lf.The transmission power, implanted antenna gain, and receiver monopole antenna gain are represented byPa, Ga, and Gb, respectively. The free space losses are represented by Lf, which may be calculated using the formula below:
(5)LdB=20log4πdλ.The distance between the implanted antenna and the external controlling device, which can range from 2 to 30 meters, is denoted byd. For the safety of patients, the European Research Council limits the input power to 25 W and the EIRPmax for the ISM (915 MHz) band to 20 dBm [15]. For the ISM (915 MHz) band, the in-body communication range was calculated. The availability of battery power and circuitry are the key problems of the IMDs. The skin implantation is considered depending on the application of the proposed antenna based on the input power. The anticipated transmission power Pt of the proposed antenna is 16 dBm, and the bit rate Br is 1 Mbps, based on the skin implanted devices. Figure 17 shows the simulated and measured link margin analysis inside skin tissue of the human body. Data at 1 Mbps might be sent across a distance of more than 15 m. It has been discovered that by altering the data rate and gain, the range of data transmission may be altered. Table 3 shows the performance comparison of the proposed work with some of the previously published relevant works.Figure 17
SAR distribution of the proposed antenna inside skin tissue over 1 g at 915 MHz.Table 3
Performance comparison of the proposed antenna with recent work.
Ref. no.Dimensions (mm3)/(λg3)Operating frequency(GHz)Realized gain (dB)Operating bandwidth(%)SAR (W/kg) @ 1 g[8]23×16.4×1.27/0.098×0.070×0.0050.402-34.912.9284.5[10]25×20×0.07/0.34×0.27×0.000952.45-16.81.221.0[11]15×21.5×1.5748/0.39×0.56×0.0392.45<-153.2Not calculated[12]3.14×100×2.54/0.082×2.6×0.0660.4/2.45-33.1/-14.5538.1/17.6241.5/149.7[14]14×14×0.5/0.365×0.365×0.0132.45-15.9618.360.494[16]3.14×28.6×1.34/0.082×0.748×0.0350.402/2.45-41/-21.341/27.8666/676[17]3.14×23×0.634/0.082×0.60×0.0162.45-20.318.3649[18]11×11×1.27/0.107×0.107×0.01230.915-293.8Not calculated[19]15×15×1.27/0.14×0.14×0.01230.915-2710.6517[20]3.14×22.09×1.27/0.030×0.22×0.01230.915-32.812.2778This work7×7×0.254/0.08×0.08×0.0030.915-2821.858.1


## 3.1. Antenna in Free Space

The designed biomedical implantable patch antenna is fabricated on a Roger RT5880 substrate with thickness of 0.254 mm and tested inside free space. A vector network analyzer (VNA) is used to measure theS11 of the implantable antenna. In the case of the simulated results, the designed antenna covers the bandwidths from 800 MHz to 1000 MHz (200 MHz) at 915 MHz while in the case of the measurements, the antenna covers the bandwidth from 795 MHz to 998 MHz (203 MHz) at 915 MHz as can be seen in Figure 8.Figure 8
(a) Measurement setup inside chamber. (b) Comparison of the simulation and measurement reflection coefficients (dB) of the patch antenna in free space.
(a)(b)TheE- and H-planes of the antenna are simulated and measured in free space (see Figure 9). The two-dimensional (2D) radiation pattern describes the behavior of the antenna. The designed antenna behaves as an omnidirectional pattern in both planes at the 915 MHz frequency band. The current density of the implantable antenna is shown in Figure 10. The current mainly flows around the upper- and bottom-sided resonators and feed patch. The red colored arrows indicate that the portion of the antenna has major contribution in operating at the desired frequency band.Figure 9
2D radiation pattern of the antenna in free space at 915 MHz.
(a)(b)Figure 10
Current distribution throughout the patch at 915 MHz.


## 3.2. Antenna inside the Skin

To explore the appropriateness of the antenna inside the skin for biomedical telemetry applications, the proposed design is simulated and tested inside skin tissue in this section. Consequently, to design an antenna for the applications in biotelemetry that had high precision, the presence of the human body phantoms must be taken into consideration while calculating SAR. For that, the antenna performance in proximity of human phantoms and the SAR values at 915 MHz are also evaluated. The area of the phantom box is20×20mm2 as can be seen in Figure 11. HFSS Studio is used for simulating the proposed antenna.Figure 11
Perspective view of the skin phantom box.In an ideal case, in-body antennas should be planned to avoid the significant coupling effects from the human tissues. While testing the antenna inside the skin of the human body, it is placed 2 mm deep inside the skin tissue as shown in Figure12. To estimate these effects, the reported design is kept inside a 40mm×40mm box of skin tissue. A “skin-mimicking gel” with relative permittivity (εr) of 43 and electrical conductivity (σ) of 1.40 is used, as its properties are very close to those of human skin tissue.Figure 12
Antenna inside the skin of human tissues: (a) perspective view, (b) fabricated prototype of the antenna, and (c) experimental setup to measure the pattern andS11.
(a)(b)(c)The contrast between the simulated and measuredS11 of the antenna inside the skin is described in Figure 13. The simulated S11 inside the skin indicates that the biomedical antenna operates from 780 MHz to 1000 MHz (220 MHz) at 915 MHz while the fabricated antenna inside the mimicking gel, on the other side, featured bandwidths from 785 MHz to 998 MHz (213 MHz). This proves that both simulated and measured results have good agreement among each other.Figure 13
Comparison between the simulated and measuredS11 of the antenna inside skin tissue.Figure14 presents the E- and H-planes of the simulation and measurement results of the radiation pattern inside skin tissue. The 2D radiation pattern describes the behavior of the antenna inside the skin. These far field results prove that the antenna inside the skin has an omnidirectional radiation pattern in both planes at the 915 MHz frequency band. The simulated realized gain value inside the skin is found to be -22 dB at 915 MHz, whereas measurement results give the realized gain of -28 dB at 915 MHz. The simulated and measured efficiency and gain graph is presented in Figure 15. The presented graph indicates that the antenna has simulated efficiency of 2.2% while the measured efficiency is 2.1% inside the skin.Figure 14
Simulated and measured far field results at 915 MHz inside skin tissue.
(a)(b)Figure 15
Simulated and measured gain and efficiency graph inside the skin.


## 3.3. Specific Absorption Rate (SAR)

The radiations of electromagnetic waves may cause health risks to the human body, and such risks are calculated in terms of SAR. The relationship between the input power and the SAR is as follows [10]:
(1)SAR=σ∣E2∣ρ,where σ and ρ denote the thermal conductivity (S/m) and the mass density (kg/m3), respectively, while E is the electric field intensity (V/m). The electric power intensity is related to the signal power as follows [13]:
(2)PowerWm2=EV/m2377.SAR simulations were accomplished when the proposed antenna is kept inside the skin as well as inside the muscle. Input power pin is kept constant at 0.5 W with the SAR evaluated based on the IEEE/IEC 6270-1 standard, averaged over 1 g of mass tissue. SAR values inside the skin are calculated as 8.17 W/kg at 915 MHz as presented in Figure16.Figure 16
SAR distribution of the proposed antenna inside skin tissue over 1 g at 915 MHz.


## 3.4. Link Budget Analysis

The telemetry range between the implanted device and the external base station must be determined in order to successfully communicate biological data. However, the link budget estimates are affected by a variety of losses, including free space losses, cable losses, and antenna material and mismatch losses [14]. The link margins were calculated using the Friis equation to calculate the difference between the antenna power (AP) and the necessary antenna power (RP), and the link margin should be more than 20 dB for consistent communication. Table 2 lists the important parameters utilized in these computations. The following formula can be used to calculate RP:
(3)RP=EbNo+KT+Br.Table 2
Parameters of the link budget of the stated design.
ParametersVariablesValueResonance frequencyfoMHz915Noise power densityNodB/Hz-203.93Transmitter powerPTxdBm-4Polarization mismatch lossPLdB1TemperatureToKelvin273Free space path lossLfdBDistance dependentTransmitter antenna gainGTxdBiScenario dependentReceiver antenna gainGRxdBi2Boltzmann constantK1.38×10−23Available powerAPdbDistance dependentBit rateBrMbps1Required powerRPdB-134.64The phase shift keying, Boltzmann’s constant, temperature, and bit rate are represented byEb/No, K, To, and Br, respectively. AP, on the other hand, may be computed as follows:
(4)APdB=Pa+Ga+Gb+Lf.The transmission power, implanted antenna gain, and receiver monopole antenna gain are represented byPa, Ga, and Gb, respectively. The free space losses are represented by Lf, which may be calculated using the formula below:
(5)LdB=20log4πdλ.The distance between the implanted antenna and the external controlling device, which can range from 2 to 30 meters, is denoted byd. For the safety of patients, the European Research Council limits the input power to 25 W and the EIRPmax for the ISM (915 MHz) band to 20 dBm [15]. For the ISM (915 MHz) band, the in-body communication range was calculated. The availability of battery power and circuitry are the key problems of the IMDs. The skin implantation is considered depending on the application of the proposed antenna based on the input power. The anticipated transmission power Pt of the proposed antenna is 16 dBm, and the bit rate Br is 1 Mbps, based on the skin implanted devices. Figure 17 shows the simulated and measured link margin analysis inside skin tissue of the human body. Data at 1 Mbps might be sent across a distance of more than 15 m. It has been discovered that by altering the data rate and gain, the range of data transmission may be altered. Table 3 shows the performance comparison of the proposed work with some of the previously published relevant works.Figure 17
SAR distribution of the proposed antenna inside skin tissue over 1 g at 915 MHz.Table 3
Performance comparison of the proposed antenna with recent work.
Ref. no.Dimensions (mm3)/(λg3)Operating frequency(GHz)Realized gain (dB)Operating bandwidth(%)SAR (W/kg) @ 1 g[8]23×16.4×1.27/0.098×0.070×0.0050.402-34.912.9284.5[10]25×20×0.07/0.34×0.27×0.000952.45-16.81.221.0[11]15×21.5×1.5748/0.39×0.56×0.0392.45<-153.2Not calculated[12]3.14×100×2.54/0.082×2.6×0.0660.4/2.45-33.1/-14.5538.1/17.6241.5/149.7[14]14×14×0.5/0.365×0.365×0.0132.45-15.9618.360.494[16]3.14×28.6×1.34/0.082×0.748×0.0350.402/2.45-41/-21.341/27.8666/676[17]3.14×23×0.634/0.082×0.60×0.0162.45-20.318.3649[18]11×11×1.27/0.107×0.107×0.01230.915-293.8Not calculated[19]15×15×1.27/0.14×0.14×0.01230.915-2710.6517[20]3.14×22.09×1.27/0.030×0.22×0.01230.915-32.812.2778This work7×7×0.254/0.08×0.08×0.0030.915-2821.858.1


## 4. Conclusion

This paper provides a low-profile ISM band compact-size patch antenna for the applications in biomedical implants. The presented antenna is simulated by using HFSS software. This proposed antenna resonates in the ISM band at 915 MHz. The antenna is designed on a Rogers material of RT/Duroid 5880 (εr=2.2, tanδ=0.0009) with complete dimensions of 7mm×7mm×0.254mm. The measured gain of the antenna inside the skin-mimicking gel is calculated as -28 dB at 915 MHz, while the measured bandwidth of the antenna reported is 21.85% inside the skin-mimicking gel. The SAR values are found to be 8.1 W/kg inside the skin. Problems of compliance with biocompatibility and safety related to the construction of medical applications were also discussed. This antenna is miniaturized and an ideal applicant for in-body biomedical applications.



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*Source: 7594587-2022-01-17.xml*