# CompactVitis vinifera-Inspired Ultrawideband Antenna for High-Speed Communications

Authors: Jeremiah O. Abolade; Dominic B. O. Konditi; Vasant M. Dharmadhikary
Journal: International Journal of Antennas and Propagation
 (2021)

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## Abstract

A new compact ultrawideband (UWB) bioinspired antenna is presented in this work. The proposed antenna consists of a vine leaf (Vitis vinifera) shape as the radiating patch, defected ground structure (DGS), and a vertical rectangular slot (VRS) on the ground plane. The vine leaf shape is realized from a circular patch (initiator) in this work. The proposed antenna is built on an FR4 substrate with a dielectric constant of 4.4, a loss tangent of 0.02, and a thickness of 1.5 mm. The total dimension of the proposed bioinspired antenna is 35 × 27.6 mm2. The proposed antenna has a fractional bandwidth of 115.43% (3.7 GHz–13.8 GHz) at 10 dB return loss, a radiation efficiency between 78% and 97%, a peak gain of 6.7 dB, and a stable radiation pattern. The contributions of this work to the existing literature are as follows: (i) the investigation of a vine leaf shape for UWB antenna application; (ii) the adaptation of the conventional monopole patch antenna design equation to determine the lower edge frequency (LEF) of an arbitrary shape monopole antenna; (iii) the presentation of a compact UWB antenna with high fractional bandwidth compared with recent works in the literature, and (iv) the use of FR4 substrate to achieve a peak radiation efficiency of 97% with a compact structure.


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## Body

## 1. Introduction

Ultrawideband antenna has attracted the attention of microwave engineers since the declaration of the Federal Communication Commission (FCC) to make it available for commercial use. This antenna readily finds application in radar, military, medical, and mobile communication. According to the FCC, the band designation for UWB is 3.1 GHz–10.6 GHz [1]. Even though this band interferes with other existing standards such as Wi-Fi, WLAN, WiMAX, and the upper ISM band, its advantages such as low power, reasonably cheaper cost of equipment, and its greater noise immunity have made it to become popular in wireless communication systems, especially in short distance communication [2, 3].Over the years, researchers have been working on how to realize a compact antenna having an ultrawide bandwidth. The printed monopole antenna is one of the major techniques being used to achieve such a wide fractional bandwidth. Some of the patch shapes commonly used in the literature are rectangular, triangular, and circular. In recent times, antenna researchers begun to look in the direction of bioinspired structure such as leave shape [4–8], the physical shape of animals [9], or internal organ shape of the animals [10] which has been explored. Authors in [4, 7] proposed a bioinspired UWB antenna based on Igna Marginata leaf. The antenna proposed in [7] has dimension of 40 × 30 mm2 and is built on an FR4 substrate of height 1.5 mm. A simulated impedance bandwidth of 9.9 GHz was achieved, but the author did not report the radiation efficiency of the antenna.The authors in [2] explored maple leaf shape to design the UWB antenna. The antenna was built on Rogers RT 5880 substrate with a relative dielectric constant of 2.2, a loss tangent of 0.0009, and a height of 1. 575 mm. The overall antenna dimension is 30.5 × 35.5 mm2 and achieves an impedance bandwidth of 3.1 GHz to 13.15 GHz with a 5GHz-6 GHz band notch. The authors also did not report the radiation efficiency. Authors in [6] presented a bioinspired antenna based on sugarcane leaf, operating at 700 MHz, and a reflector was used to enhance the gain of the proposed antenna. In [11], the authors investigated Tulip flower shape having a dimension 56.25 × 35.7 mm2 for UWB application, and impedance bandwidth of 9.45 GHz was achieved. Jasmine flower, Ginkgo Biloba, Carica Papaya, and Bidens Pilosa leaves have been designed, fabricated, and analyzed for UWB applications.The radiation efficiency of an antenna is a critical antenna performance metric in mobile applications where omnidirectional radiation is essential. This is because, radiation efficiency, unlike gain, is a measure of antenna performance without considering the direction of radiation. Notwithstanding, none of the bioinspired UWB antennas in the open literature gives much attention to the radiation efficiency of the reported antennas.Therefore, in the quest for increased UWB bandwidth and enhanced efficiency, this work investigates vine leaf (Vitis vinifera) shape as a bioinspired structure for UWB wireless applications. The motivation behind this investigation is the sawtooth edge of the vine leaf. In the next section, the vine leaf shape antenna design procedure is presented and then the shape was used as the radiating patch. Section 3 presents the parametric study of the proposed antenna; the measurement results are presented in Section 4; the comparative analysis of the proposed antenna with the relevant existing work in the open literature is presented in Section 5, and the conclusion is presented in Section 6.


## 2. Antenna Design Procedure

The radiating patch of the proposed antenna is based on vine leaf shape on an epoxy glass (FR4) substrate of a dielectric constant of 4.4, a loss tangent of 0.02, and a height of 1.5 mm with a defected ground structure (DGS) and a vertical rectangular (VR) slot as the ground plane. The proposed antenna is fed with a50Ω feedline. The proposed antenna dimension is 35 × 27.6 mm2. Figure 1 shows the picture of a typical vine leaf. The proposed antenna shall hereafter be referred to as vine bioinspired UWB antenna (VBi-UWBA).Figure 1
A typical vine leaf shape.The initiator of the VBi-UWBA structure is a circular shape. A circular patch of radius (r) 10 mm is chosen as the initiator as shown in Figure 2(a) to achieve a lower edge frequency (LEF) around 3 GHz using equation (1) which is adapted from reference [12]. As shown in Figure 1, the vine leaf has saw-like edges and the circular shape edge is perturbed to achieve a saw-like edge as shown in Figure 2(b). Hence, the maximum edge length of the VBi-UWBA radiating patch from its center is 10 mm as demonstrated in Figure 2(b). Using the area of a circle given in equation (2), the area of the initiator is 314.2 mm2 but the area of the resultant vine leaf shape is measured to be 221.32 mm2 using the measurement tool of the HFSS simulator. This implies that the resultant radius is 8.39 mm. A 16.1% reduction is achieved compared with the initiator (CMPA). Using the resultant radius to determine the LEF of the vine leaf shape from equation (1), a LEF of 3.22 GHz is expected compared with 3 GHz of the CMPA. Meanwhile, the lower antenna resonant frequency has also been related to its radiating patch perimeter using equations (3) and (4) in reference [5].(1)fl=0.24×300D+g+D/2π×kGHz,(2)area of a circleA=πr2,(3)frGHz=300φεeff,(4)εeff≈εr+12,where D is the diameter of the circle in millimeter, g is the gap between the edge of the radiating patch and the ground plane in millimeter, εr is the dielectric constant of the substrate, φ is the perimeter of the patch, fr is the resonant frequency, and k accounts for the effect of dielectric permittivity of the substrate, and it is taken to be 1.15 [12].Figure 2
Vine leaf shape realization procedure: (a) the initiator circular patch; (b) the realized vine leaf shape.
(a)(b)The proposed VBi-UWBA geometry is presented in Figure3. Table 1 presents the XY-points coordinates of the proposed Vitis vinifera leaf radiating patch which are extracted from the graphing technique for repeatability purposes.Figure 3
Proposed compact bioinspired UWB antenna.Table 1
The point coordinates of the proposedVitis vinifera leaf-shaped radiating patch.
Semi-vine leaf coordinate pointsNXyNxyNXy1−10.00.0357.85.969−2.8−8.02−8.00.9367.64.170−3.8−8.23−8.41.1378.84.971−3.8−7.44−7.01.5388.63.572−6.0−8.05−7.61.9399.02.973−3.4−4.26−6.22.3408.01.974−5.0−5.27−6.62.9418.61.775−4.6−4.08−5.03.5424.80.076−6.8−4.69−5.84.5439.6−1.677−5.4−2.910−4.04.9448.4−2.278−6.6−3.311−4.65.34510.6−2.979−6.2−2.512−2.64.7469.2−3.380−7.4−2.713−3.45.74710.0−3.981−6.8−1.814−3.05.9489.2−4.082−7.8−2.215−3.66.9499.0−5.083−7.6−1.416−3.06.9507.8−4.884−8.4−1.617−3.68.9517.6−6.785−8.0−0.818−2.48.1526.6−6.119−2.68.7535.8−7.420−1.68.1545.4−7.021−1.68.7555.0−7.622−0.27.7564.8−7.2230.28.5573.8−8.0241.47.7583.6−6.1251.68.1593.2−6.5262.07.5603.2−7.6272.38.5612.8−7.4283.86.9621.8−8.6293.48.1631.0−8.0305.07.3640.4−8.6315.47.7650.2−8.0325.86.766−1.0−8.9336.27.167−1.6−8.0347.05.568−2.4−8.6The design parameters labeled in Figure4 are as presented in Table 2.Figure 4
The VBi-UWBA separating the radiating patch from the substrate and ground plane.Table 2
VBi-UWBA optimal design parameters.
S/NParameterDescriptionValue (mm)1WsubWidth of the substrate27.62LsubLength of the substrate35.03LsLength of the slot on the ground6.04wsWidth of the slot on the ground2.1825LgLength of the ground plane10.06WfWidth of the feedline2.87LfLength of the feedline12.38rRadius of the initiator10.09gSeparation between patch and ground0.00


## 3. Parametric Study and Analysis of VBi-UWBA

In this section, the parametric analysis of VBi-UWBA is presented. This is done to evaluate the effect of the design parameters on the resonant frequency.


### 3.1. The Effect of the Length of the Defected GroundLg

To evaluate the effect ofLg, the slot was eliminated and Lg varies from 20 mm to 5 mm with an interval of 3 mm. The response is as shown in Figure 5. It can be observed that the length of the ground plane has a tremendous effect on the performance of the proposed structure. It can be seen that a UWB with a –10 dB fractional bandwidth of 118.1% (3.21 GHz–12.47 GHz) can be achieved only when Lg  = 10 mm. When Lg  = 11 mm, the reflection coefficient response demonstrates a UWB with a bandgap between 8.41 GHz and 9.46 GHz. For Lg=5mm, the first resonance mode is at 2.87 GHz which is the lowest resonant mode of all the Lg variation.Figure 5
Effect ofLg variation on the reflection coefficient.It can be observed that asLg increases, the fundamental resonance frequency increases. This effect can be traced to the change in the antenna impedance matching with the 50 Ω feedline because as the capacitive reactance formed by the dielectric-filled gap between the radiating patch and the ground varies with the variation in the length of the ground plane, there is a corresponding variation in the overall antenna impedance which can cause impedance mismatch. It can also be observed that as Lg increases from 5 mm to 14 mm, the LEF is simultaneously increasing. Notwithstanding, LEF starts decreasing again from Lg = 17 mm and above. Therefore, Lg can be used for tuning the LEF of a monopole antenna. Because the focus of this work is UWB, the optimized Lg is therefore taken to be 10 mm based on this parametric analysis.


### 3.2. The Effect of Slot Length (Ls)

Figure6 shows the effect of Ls on reflection coefficient while keeping Lg and Ws at 10 mm and 2.18 mm, respectively. It is observed that the VR slot on the ground plane affects the return loss at the resonance rather than creating another resonance at a new frequency. It is can be seen that at the lower resonance frequency, the best return loss (31.3 dB) is achieved when Ls = 4 mm. Notwithstanding, at this value of Ls, the return loss is relatively poor around 9.2 GHz compared with when it is 3 mm, 5 mm, and 6 mm.Figure 6
Effect ofLs variation on the reflection coefficient.It can be seen that, though, the return loss response whenLs = 6 mm is saggy from 3.22 GHz to 12.47 GHz. Hence, 6 mm is chosen as the optimized value of Ls. It is observed that slot in the ground plane enhances the return loss which is a result of matching the antenna impedance to the feedline impedance by reducing the capacitive reactance introduced by the feedline and thereby enhances the impedance matching of the antenna.


### 3.3. The Effect of Slot Width (Ws)

The effect of the slot width of the ground plane is presented in Figure7. It can be seen that Ws has almost the same effect as the slot length. It is observed that UWB is achievable at 1 mm, 1.5 mm, 2 mm, and 2.182 mm values of Ws without a notch between 3.1 GHz–12.38 GHz, respectively. Meanwhile, 2.5 mm and 3.25 mm values of Ws demonstrate a band notch within the UWB between 8.55 GHz and 9.60 GHz. 2.182 mm gives a better return loss response. Hence, the optimized parameter of Ws is taken to be 2.182 mm. It is noted that Ws does not have a considerable effect on the LEF of the proposed structure but there is a notable effect on the return loss. Hence, the width of the slot can be used to enhance the return loss of VBi-UWBA.Figure 7
Effect ofWs variation on the reflection coefficient.Therefore, the optimized value of the defected ground plane is given in Table2.


## 3.1. The Effect of the Length of the Defected GroundLg

To evaluate the effect ofLg, the slot was eliminated and Lg varies from 20 mm to 5 mm with an interval of 3 mm. The response is as shown in Figure 5. It can be observed that the length of the ground plane has a tremendous effect on the performance of the proposed structure. It can be seen that a UWB with a –10 dB fractional bandwidth of 118.1% (3.21 GHz–12.47 GHz) can be achieved only when Lg  = 10 mm. When Lg  = 11 mm, the reflection coefficient response demonstrates a UWB with a bandgap between 8.41 GHz and 9.46 GHz. For Lg=5mm, the first resonance mode is at 2.87 GHz which is the lowest resonant mode of all the Lg variation.Figure 5
Effect ofLg variation on the reflection coefficient.It can be observed that asLg increases, the fundamental resonance frequency increases. This effect can be traced to the change in the antenna impedance matching with the 50 Ω feedline because as the capacitive reactance formed by the dielectric-filled gap between the radiating patch and the ground varies with the variation in the length of the ground plane, there is a corresponding variation in the overall antenna impedance which can cause impedance mismatch. It can also be observed that as Lg increases from 5 mm to 14 mm, the LEF is simultaneously increasing. Notwithstanding, LEF starts decreasing again from Lg = 17 mm and above. Therefore, Lg can be used for tuning the LEF of a monopole antenna. Because the focus of this work is UWB, the optimized Lg is therefore taken to be 10 mm based on this parametric analysis.


## 3.2. The Effect of Slot Length (Ls)

Figure6 shows the effect of Ls on reflection coefficient while keeping Lg and Ws at 10 mm and 2.18 mm, respectively. It is observed that the VR slot on the ground plane affects the return loss at the resonance rather than creating another resonance at a new frequency. It is can be seen that at the lower resonance frequency, the best return loss (31.3 dB) is achieved when Ls = 4 mm. Notwithstanding, at this value of Ls, the return loss is relatively poor around 9.2 GHz compared with when it is 3 mm, 5 mm, and 6 mm.Figure 6
Effect ofLs variation on the reflection coefficient.It can be seen that, though, the return loss response whenLs = 6 mm is saggy from 3.22 GHz to 12.47 GHz. Hence, 6 mm is chosen as the optimized value of Ls. It is observed that slot in the ground plane enhances the return loss which is a result of matching the antenna impedance to the feedline impedance by reducing the capacitive reactance introduced by the feedline and thereby enhances the impedance matching of the antenna.


## 3.3. The Effect of Slot Width (Ws)

The effect of the slot width of the ground plane is presented in Figure7. It can be seen that Ws has almost the same effect as the slot length. It is observed that UWB is achievable at 1 mm, 1.5 mm, 2 mm, and 2.182 mm values of Ws without a notch between 3.1 GHz–12.38 GHz, respectively. Meanwhile, 2.5 mm and 3.25 mm values of Ws demonstrate a band notch within the UWB between 8.55 GHz and 9.60 GHz. 2.182 mm gives a better return loss response. Hence, the optimized parameter of Ws is taken to be 2.182 mm. It is noted that Ws does not have a considerable effect on the LEF of the proposed structure but there is a notable effect on the return loss. Hence, the width of the slot can be used to enhance the return loss of VBi-UWBA.Figure 7
Effect ofWs variation on the reflection coefficient.Therefore, the optimized value of the defected ground plane is given in Table2.


## 4. Results and Discussion

The prototype of the proposed antenna is as shown in Figure8. Figure 8(a) shows the top layer (the vine radiating patch and the feedline), and the ground plane is shown in Figure 8(b). The reflection coefficient measurement setup is as shown in Figure 9. The Rhode and Schwaz ZVA50 Vector Network Analyzer is used for the reflection coefficient measurement of the proposed VBi-UWBA.Figure 8
The prototype of the proposed VBi-UWBA (a) top layer and (b) ground plane.
(a)(b)Figure 9
The measurement setup for reflection coefficient of the VBi-UWBA.


### 4.1. Simulated and Measured Reflection Coefficient

Figure10 shows the simulated and measured reflection coefficient of the proposed bioinspired UWB antenna. It can be seen from the simulation that the VBi-UWBA has a fractional bandwidth of 117.9% (3.26 GHz–12.62 GHz) at a return loss of 10 dB. It can be observed that the LEF of the simulation (3.26 GHz) agrees with the LEF predicted (3.22 GHz) in Section 2. In the case of the measurement, the proposed antenna demonstrated UWB with a fractional bandwidth of 115.43% (3.7 GHz–13.8 GHz) at −10 dB.Figure 10
Reflection coefficient of VBi-UWBA.The shift in the LEF in the measurement can be traced to the effect of the SMA connector and the soldering. Nonetheless, both simulated and measured impedance bandwidth at −10 dB is in good agreement. The measurement result of the proposed VBi-WBA shows that it is well suitable for UWB application as it covers the entire band allocated for UWB and outperforms the existing bioinspired UWB antennas reported in the open literature.


### 4.2. Radiation Pattern

The radiation pattern of the proposed VBi-UWBA is investigated at 4.5 GHz, 5.5 GHz, 7.5 GHz, 10.5 GHz, and 13.5 GHz which are presented as shown in Figures11(a)–11(e), respectively. It can be observed that the radiation pattern at 4.5 GHz and 5.5 GHz is bidirectional in XZ-plane while the XZ-plane radiation patterns at 7.5 GHz, 10.5 GHz, and 13.5 GHz are quasi-omnidirectional. At YZ-plane, the radiation patterns are omnidirectional in all the investigated frequencies.Figure 11
Simulated radiation pattern of proposed VBi-UWBA.
(a)(b)(c)(d)(e)At 4.5 GHz, the direction of the main lobe is at176° and the angular width (3 dB) is 112° for XZ-plane as shown in Figure 11(a). As can be seen in Figure 11(b), the 5.5 GHz XZ-plane radiation pattern has its main lobe direction at 166° and the 3 dB angular width is 106°. Furthermore, at 7.5 GHz, the main lobe direction is at 16° and the 3 dB angular width is 78° at XZ-plane as shown in Figure 11(c). As shown in Figure 11(d), at 10.5 GHz, the main lobe direction is at 30° and the angular width (3 dB) is 54° at XZ-plane. In the case of 13.5 GHz, the main lobe direction is at 68° and its 3 dB angular width is 56° as shown in Figure 11(e). Hence, the proposed VBi-UWBA has a stable radiation pattern through the entire bandwidth. These characteristics make VBi-UWBA a good candidate for mobile applications.


### 4.3. The Gain and Radiation Efficiency of the Proposed VBi-UWBA

Antenna gain shows how well the antenna radiates energy in a particular direction, but radiation efficiency shows how well an antenna utilizes the received power for radiation in all directions. Equations (5) and (6) present the theoretical formula for gain and radiation efficiency, respectively. The gain of VBi-UWBA at 4.5Ghz,5.5GHz,7.5GHz,10.5GHz,and13.5GHz is presented in Figure 12. A peak gain of 2.9 dB, 3.5 dB, 4.7 dB, 3.4 dB, and 6.7 dB is achieved at 4.5Ghz,5.5GHz,7.5GHz,10.5GHz,and13.5GHz, respectively. This shows that the proposed antenna has a suitable gain across the UWB.Figure 12
The simulated 3D gain of the proposed VBi-UWBA at (a) 4.5 GHz, (b) 5.5 GHz, (c) 7.5 GHz, (d) 10.5 GHz, and (e) 13.5 GHz.
(a)(b)(c)(d)(e)The radiation efficiency and the axial ratio of the proposed VBi-UWBA are presented in Figure13. It can be observed that the proposed antenna demonstrates high radiation efficiency ranging from 78% to 97%. As far as we know, this is the highest peak radiation efficiency reported in the literature for compact UWB antenna applications with FR4 substrate. It can be observed in Figure 13 that at 11.5 GHz, the proposed VBi-UWBA demonstrates circular polarization with a 2.2% 3dB axial ratio bandwidth (ARBW).(5)Gφ,θ=4πUφ,θPin,(6)e=RrRr+RL,where Gφ,θis the total gain,eis the efficiency,Uφ,θ is the radiation intensity, Pinis the total input power,Rris the radiation resistance,andRLis the radiation losses.Figure 13
The simulated radiation efficiency and the axial ratio of the proposed VBi-UWBA.


### 4.4. The Current Distribution of VBi-UWBA

In order to have a full understanding of the operation of the proposed VBi-UWBA, a study of its current distribution is performed and presented in this section. From Section3.1, it can be observed that there are four excitation modes which occur at 4.6 GHz, 8 GHz, 10.8 GHz, and 11.5 GHz, respectively. Therefore, the investigation of the mode of operation of the proposed VBi-UWBA is done at these frequencies using its surface current distribution. Figure 14 shows the current distribution at the aforesaid frequencies.Figure 14
Simulated vector surface current distribution of the proposed VBi-UWBA at (a) 4.6 GHz, (b) 8 GHz, (c) 10.8 GHz, and (d) 11.5 GHz.
(a)(b)(c)(d)The current distribution of the fundamental mode is as shown in Figure14(a). It can be observed that the current flows toward the top tip of the radiating patch with the higher density current flowing along the edge. In addition, at the ground plane, the current flows toward the edge of the VR slot to near the radiating patch. This excitation mode is equivalent to the fundamental mode (TE11) of a circular patch (initiator). The calculated resonant frequency of this mode is 4.7 GHz using the circular patch antenna design equation given as follows, which agrees with the computation result:(7)fnm=XnmC2πaeεr,(8)ae=a1+2hπaεrInπa2h+1.7726,where a is the radius of the radiating patch which in our case is 8.39 mm and Xnm is the mth zero of the derivative of Jnka.Figure14(b) shows the current distribution at 8 GHz; it can be observed that different modes are excited which leads to a null at the center of the radiating patch. This scenario justifies why the resonance at this frequency almost disappeared. At this frequency, the current is seen to be flowing towards the two bottom edges of the ground plane.The current distribution at 10.8 GHz is as shown in Figure14(c). Just like in the case of 8 GHz, many modes are excited by the antenna and therefore a null can be observed at the center of the radiating patch as well as the two halves of the ground plane, hence poor resonance. At 11.5 GHz, the current distribution is seen to be rotating in with time. Therefore, circular polarization is achieved at this frequency. The CP achieved at this frequency (11.5 GHz) is due to the excitation of two linear modes with a 90° phase shift as seen in Figure 14. This could be traced to the asymmetric topology of the Vitis vinifera leaf-shaped and not the feeding technique [13]. With this analysis, it can be clearly stated that excitation of several modes which are added constructively leads to the UWB nature of the proposed VBi-UWBA in this work.


### 4.5. Group Delay of VBi-UWBA

Group delay is another performance metric of the UWB antenna which shows the degree of distortion between the antenna transmitting and the receiving antenna. In order to evaluate the group delay of VBi-UWBA, a face-to-face configuration of two VBi-UWBAs is set up at 300 mm apart for the far-field scenario as shown in Figure15. It can be seen from Figure 16 that the group delay of VBi-UWBA is around 0.1 ns from 3 GHz to 12.4 GHz. There is a little spike to 1.2 ns at 13.2 GHz but which is still within the acceptable limit. Hence, there is a negligible distortion in the signal of the UWB system. With this analysis, the proposed VBi-UWBA is suitable for high-speed UWB communication.Figure 15
Face-to-face configuration of two VBi-UWBAs.Figure 16
Simulated group delay of VBi-UWBA.


## 4.1. Simulated and Measured Reflection Coefficient

Figure10 shows the simulated and measured reflection coefficient of the proposed bioinspired UWB antenna. It can be seen from the simulation that the VBi-UWBA has a fractional bandwidth of 117.9% (3.26 GHz–12.62 GHz) at a return loss of 10 dB. It can be observed that the LEF of the simulation (3.26 GHz) agrees with the LEF predicted (3.22 GHz) in Section 2. In the case of the measurement, the proposed antenna demonstrated UWB with a fractional bandwidth of 115.43% (3.7 GHz–13.8 GHz) at −10 dB.Figure 10
Reflection coefficient of VBi-UWBA.The shift in the LEF in the measurement can be traced to the effect of the SMA connector and the soldering. Nonetheless, both simulated and measured impedance bandwidth at −10 dB is in good agreement. The measurement result of the proposed VBi-WBA shows that it is well suitable for UWB application as it covers the entire band allocated for UWB and outperforms the existing bioinspired UWB antennas reported in the open literature.


## 4.2. Radiation Pattern

The radiation pattern of the proposed VBi-UWBA is investigated at 4.5 GHz, 5.5 GHz, 7.5 GHz, 10.5 GHz, and 13.5 GHz which are presented as shown in Figures11(a)–11(e), respectively. It can be observed that the radiation pattern at 4.5 GHz and 5.5 GHz is bidirectional in XZ-plane while the XZ-plane radiation patterns at 7.5 GHz, 10.5 GHz, and 13.5 GHz are quasi-omnidirectional. At YZ-plane, the radiation patterns are omnidirectional in all the investigated frequencies.Figure 11
Simulated radiation pattern of proposed VBi-UWBA.
(a)(b)(c)(d)(e)At 4.5 GHz, the direction of the main lobe is at176° and the angular width (3 dB) is 112° for XZ-plane as shown in Figure 11(a). As can be seen in Figure 11(b), the 5.5 GHz XZ-plane radiation pattern has its main lobe direction at 166° and the 3 dB angular width is 106°. Furthermore, at 7.5 GHz, the main lobe direction is at 16° and the 3 dB angular width is 78° at XZ-plane as shown in Figure 11(c). As shown in Figure 11(d), at 10.5 GHz, the main lobe direction is at 30° and the angular width (3 dB) is 54° at XZ-plane. In the case of 13.5 GHz, the main lobe direction is at 68° and its 3 dB angular width is 56° as shown in Figure 11(e). Hence, the proposed VBi-UWBA has a stable radiation pattern through the entire bandwidth. These characteristics make VBi-UWBA a good candidate for mobile applications.


## 4.3. The Gain and Radiation Efficiency of the Proposed VBi-UWBA

Antenna gain shows how well the antenna radiates energy in a particular direction, but radiation efficiency shows how well an antenna utilizes the received power for radiation in all directions. Equations (5) and (6) present the theoretical formula for gain and radiation efficiency, respectively. The gain of VBi-UWBA at 4.5Ghz,5.5GHz,7.5GHz,10.5GHz,and13.5GHz is presented in Figure 12. A peak gain of 2.9 dB, 3.5 dB, 4.7 dB, 3.4 dB, and 6.7 dB is achieved at 4.5Ghz,5.5GHz,7.5GHz,10.5GHz,and13.5GHz, respectively. This shows that the proposed antenna has a suitable gain across the UWB.Figure 12
The simulated 3D gain of the proposed VBi-UWBA at (a) 4.5 GHz, (b) 5.5 GHz, (c) 7.5 GHz, (d) 10.5 GHz, and (e) 13.5 GHz.
(a)(b)(c)(d)(e)The radiation efficiency and the axial ratio of the proposed VBi-UWBA are presented in Figure13. It can be observed that the proposed antenna demonstrates high radiation efficiency ranging from 78% to 97%. As far as we know, this is the highest peak radiation efficiency reported in the literature for compact UWB antenna applications with FR4 substrate. It can be observed in Figure 13 that at 11.5 GHz, the proposed VBi-UWBA demonstrates circular polarization with a 2.2% 3dB axial ratio bandwidth (ARBW).(5)Gφ,θ=4πUφ,θPin,(6)e=RrRr+RL,where Gφ,θis the total gain,eis the efficiency,Uφ,θ is the radiation intensity, Pinis the total input power,Rris the radiation resistance,andRLis the radiation losses.Figure 13
The simulated radiation efficiency and the axial ratio of the proposed VBi-UWBA.


## 4.4. The Current Distribution of VBi-UWBA

In order to have a full understanding of the operation of the proposed VBi-UWBA, a study of its current distribution is performed and presented in this section. From Section3.1, it can be observed that there are four excitation modes which occur at 4.6 GHz, 8 GHz, 10.8 GHz, and 11.5 GHz, respectively. Therefore, the investigation of the mode of operation of the proposed VBi-UWBA is done at these frequencies using its surface current distribution. Figure 14 shows the current distribution at the aforesaid frequencies.Figure 14
Simulated vector surface current distribution of the proposed VBi-UWBA at (a) 4.6 GHz, (b) 8 GHz, (c) 10.8 GHz, and (d) 11.5 GHz.
(a)(b)(c)(d)The current distribution of the fundamental mode is as shown in Figure14(a). It can be observed that the current flows toward the top tip of the radiating patch with the higher density current flowing along the edge. In addition, at the ground plane, the current flows toward the edge of the VR slot to near the radiating patch. This excitation mode is equivalent to the fundamental mode (TE11) of a circular patch (initiator). The calculated resonant frequency of this mode is 4.7 GHz using the circular patch antenna design equation given as follows, which agrees with the computation result:(7)fnm=XnmC2πaeεr,(8)ae=a1+2hπaεrInπa2h+1.7726,where a is the radius of the radiating patch which in our case is 8.39 mm and Xnm is the mth zero of the derivative of Jnka.Figure14(b) shows the current distribution at 8 GHz; it can be observed that different modes are excited which leads to a null at the center of the radiating patch. This scenario justifies why the resonance at this frequency almost disappeared. At this frequency, the current is seen to be flowing towards the two bottom edges of the ground plane.The current distribution at 10.8 GHz is as shown in Figure14(c). Just like in the case of 8 GHz, many modes are excited by the antenna and therefore a null can be observed at the center of the radiating patch as well as the two halves of the ground plane, hence poor resonance. At 11.5 GHz, the current distribution is seen to be rotating in with time. Therefore, circular polarization is achieved at this frequency. The CP achieved at this frequency (11.5 GHz) is due to the excitation of two linear modes with a 90° phase shift as seen in Figure 14. This could be traced to the asymmetric topology of the Vitis vinifera leaf-shaped and not the feeding technique [13]. With this analysis, it can be clearly stated that excitation of several modes which are added constructively leads to the UWB nature of the proposed VBi-UWBA in this work.


## 4.5. Group Delay of VBi-UWBA

Group delay is another performance metric of the UWB antenna which shows the degree of distortion between the antenna transmitting and the receiving antenna. In order to evaluate the group delay of VBi-UWBA, a face-to-face configuration of two VBi-UWBAs is set up at 300 mm apart for the far-field scenario as shown in Figure15. It can be seen from Figure 16 that the group delay of VBi-UWBA is around 0.1 ns from 3 GHz to 12.4 GHz. There is a little spike to 1.2 ns at 13.2 GHz but which is still within the acceptable limit. Hence, there is a negligible distortion in the signal of the UWB system. With this analysis, the proposed VBi-UWBA is suitable for high-speed UWB communication.Figure 15
Face-to-face configuration of two VBi-UWBAs.Figure 16
Simulated group delay of VBi-UWBA.


## 5. Comparative Analysis of VBi-UWBA with Recent Works in the Literature

Table3 presents the comparative analysis of the VBi-UWBA structure with the existing works in the literature. Though the antenna proposed in [1, 4, 8, 16, 22, 23] is comparatively small than the proposed antenna in this work, it was observed that the peak gain of the proposed antenna is higher than the peak gain reported by the authors and the radiation efficiency is not reported. The antenna proposed in this work is comparatively compact than the antenna reported in [15, 17, 19, 24, 25] as shown in Table 3. Although the proposed antenna in [20] has a compact size nonetheless with a peak group delay and minimum radiation efficiency of 4 ns and 35% while in this work, a peak group delay and minimum radiation efficiency are 1.1 ns and 78%, respectively. It can be observed that the antenna proposed in [21] has a similar size to the antenna proposed in this work but with a lesser peak gain. It can be observed that VBi-UWBA outperformed the reported bioinspired UWB antennas in terms of size, fractional bandwidth, peak gain, and radiation efficiency. Therefore, the proposed VBi-UWBA is well suitable for high-speed UWB applications.Table 3
Comparative analysis of VBi-UWBA with the existing literature.
RefSize (λ02)Substratefl/fh (GHz)Peak gain (dB)Rad. efficiency (%)[14]0.4 × 0.4RT Duroid 58803/10.84.7NR[15]0.5 × 0.4FR43.1/10.65.2NR[16]0.2 × 0.2FR41.4/11.34.6NR[17]0.4 × 0.4Arlon Diclad 880A1.79/28.028.0NR[1]0.4 × 0.2FR43/10.6NRNR[8]0.4 × 0.2FR41.9/6.210.2NR[18]0.3 × 0.2FR41.8/124.078–96[19]0.4 × 0.4FR42.8/145.075–90[4]0.3 × 0.3FR40.5/1.52.81NR[7]0.4 × 0.3FR42.74/136.2dBiNR[20]0.1 × 0.2FR43.07–11.65.535–90[21]0.4 × 0.3FR42.9/154.590∗[22]0.2 × 0.2FR43/204.070∗[23]0.3 × 0.3FR43.05/11.95.994+[24]0.4 × 0.5FR43.1/10.62.5NRThis work0.4 × 0.3FR43.7/13.86.778–97NR: not reported;∗indicates average value; +indicates total value.


## 6. Conclusion

A novel compact bioinspired UWB antenna is investigated in this work. A conventional monopole antenna design formula is adapted to determine the LEF of the proposed bioinspired antenna in this work. The analysis result and computation result agree. The measurement agrees with the simulation result. The proposed VBi-UWBA has a fractional bandwidth of 115.43% at a 10 dB return loss, a suitable gain across the wideband, a high radiation efficiency, and a stable omnidirectional radiation pattern which make it a suitable candidate for UWB wireless applications such as sensing, imaging, ground-penetration radar, and personal area network (PAN).



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*Source: 9975884-2021-05-18.xml*