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Research & Development in Material Science
242
Res Dev Material Sci
242
Introduction
The Vivaldi antenna is a special kind of tapered slot antenna
(TSA), having an exponentially tapered slot profile. It is first
recognized by Gibson in 1979 [1-3]. It is useful for wide-band
applications [4]. This research focused mainly on miniature
antennas with a low losses and high gain. The aim of this research
is to compute the far-field pattern and to compute the impedance
matching of the structure [5,6] (Figure 1).
Sunita Rani, Himanshu Monga* and Silki Baghla
Department of ECE, JCDM College of Engineering, India
*Corresponding author: Himanshu Monga, Department of ECE, Sirsa, India
Submission: December 04, 2017; Published: January 25, 2018
Design and Performance Enhancement of
Vivaldi Antenna
Copyright © All rights are reserved by Himanshu Monga.
Abstract
In this paper, a computer aided design of Vivaldi Antenna is developed which is used to study the effect of different parameters such as rate of
opening of exponential slot and size of the radius of circular slot of the Vivaldi Antenna. The proposed design resulted in enhancement of gain and
reduction in reflection losses. COMSOL Multi physics simulator is used to design the proposed Vivaldi antenna.
Keywords: Vivaldi Antenna; COMSOL Multiphysics; Copper Plate (FR4, 3.38 dielectric value)
Figure 1: Vivaldi antenna structure.
The proposed Vivaldi antennas consist of a micro strip feed line,
micro strip line to slot line transition, and the radiating structure.
Radiating structure is exponential tapered and the radiation takes
place along the axis of the tapering [7-9]
This antenna comprises of three different types of slot lines
which are:
a. The circular slot which is used to realize the impedance
matching of the micro strip transmission line.
b. The rectangular slot which is used to couple the
electromagnetic wave from the micro strip transmission line.
c. The exponential tapered slot which is used.
In this Vivaldi antenna model, the tapered slot is patterned
with a prefect electric conductor (PEC) ground plane the top of the
Short Communication
Research & Development in
Material Science
C CRIMSON PUBLISHERS
Wings to the Research
ISSN: 2576-8840
How to cite this article: Sunita R, Himanshu M, Silki B. Design and Performance Enhancement of Vivaldi Antenna. Res Dev Material Sci. 3(2). RDMS.000560.
2018. DOI: 10.31031/RDMS.2018.03.000560
243
Res Dev Material Sci
Research & Development in Material Science
dielectric substrate. One end of the slot is open to the air and other
end is finished with a circular slot. On the bottom of the substrate,
the shorted 50Ohm micro strip feed line is modeled PEC surface.
The entire molding domain is bounded by perfectly matched layer
(PEC) which act like an chamber absorbing all radiated energy.
Related Work
Dhawan [1] Presented the design and detailed results of the
Vivaldi Antenna with the selection of FR4(2.33) substrate material.
This antenna is showing remarkable performance at a frequency
of 7.5GHz and VSWR equal to-24.5dB with high directivity and
narrow beam width. Ying [3] proposed one design that starts from
a single balanced Vivaldi antenna unit, designs and analyses the
electromagnetic characteristics of balanced Vivaldi antenna array.
Then get a high-gain more than 35dB successfully by a parabolic
antenna with the feed of 4 × 3 × 3 Vivaldi array. ANU [8] designed
an antenna which used in the band from 2.1GHz to 9.2GHz with
a fractional bandwidth of 125.66%. Corresponding to the design
frequency of 2.8GHz a peak gain of 6.122dB and minimum S11 of
-28.5dB is achieved [10-12].
Design Parameters of Proposed Antenna
General parameters that are used during the design of Vivaldi
are given in Table 1.
Table 1: Design parameters.
Name Expression Value Description
W-slot 0.5 [mm] 5.000E-4 m Slot width
Thickness 60 [mil] 0.0015240 m Substrate thickness
F-max 6.0 [GHz] 6.0000E9 Hz
Maximum Frequency in
sweep
F-min 2.0 [GHz] 2.0000E9Hz
Minimum frequency in
sweep
F0 F-max 6.5000E9 Hz Current frequency in sweep
Length 110 [mm] 011000 m Length of antenna
Radius 10 [mm] 0.012000 m Radius of circular slot
Width 80 [mm] 0.080000 m Width of antenna
Dielectric 3.38 33800
Dielectric constant of
substrate
Design Procedure
The proposed VIVALDI antenna is designed using COMSOL
simulate with following step:
a. Select the dimensions.
b. The Vivaldi antenna is realized on a thin dielectric substrate.
The Vivaldi block with the dimensions given in Table 1 is drawn
on substrate FR4. The length of the Vivaldi antenna is 110mm,
thickness is 1.5mm and breadth is 80mm Figure 2.
Figure 2: Substrate.
c. In the next step, feed line is selected. In this work the feed line with the line width=3.2, Depth=0+w_slot/2, Height =thickness
breadth of 5mm and length 16mm is drawn. Shown in Figure 3.
Figure 3: Feed line.
How to cite this article: Sunita R, Himanshu M, Silki B. Design and Performance Enhancement of Vivaldi Antenna. Res Dev Material Sci. 3(2). RDMS.000560.
2018. DOI: 10.31031/RDMS.2018.03.000560
Research & Development in Material Science
244
Res Dev Material Sci
d. Under a plane geometry node we define and create the
geometry sequence for a work plane. The plane geometry node
also contains some settings for the visualization of the work plane’s
geometry. Plane geometry for the proposed antenna with the radius
of 10mm is show in Figure 4.
e. Apply electromagnetic wave in frequency domain and the
antenna is made up of FR4 material with electrical permeability
Figure 4-6.
Figure 4: Plane geometry.
Figure 5: Electromagnetic waves, frequency domain.
Figure 6: Mesh.
f. In this step, the antenna will be divided into small part. A
mesh imported into COMSOL can be used to construct geometry.
Discussion & Results
The proposed antenna is analyzed with variation in radius
and it is found that at radius of 10mm. The designed antenna
provides maximum electric field of 64 as show in Figure 7. When
How to cite this article: Sunita R, Himanshu M, Silki B. Design and Performance Enhancement of Vivaldi Antenna. Res Dev Material Sci. 3(2). RDMS.000560.
2018. DOI: 10.31031/RDMS.2018.03.000560
245
Res Dev Material Sci
Research & Development in Material Science
then electric field of Vivaldi antenna is 64 the designed antenna
promotes the gain from 7.95dB in the desired frequency band (2
to 6.5GHz) as shown in Figure 8. The improved antenna gain can be
used for applications like microwave imaging and radars. The result
of our simulation can be seen in the form of SWR plot. According
to our result SWR parameter is minimum 1.14 at 3.5GHz as shown
in Figure 9 & Figure 10 Show the Far field radiation pattern for
FR4, beginning frequency is 2GHz and 6.5GHz that is the finish
frequency. In this far field, radiation pattern diagram highest output
frequency at 4.5GHz. With the selection of feed purpose employed
in this model, the S11 parameter is minimum at 3.5GHz as shown
in Figure 11 & Figure 12 shows a good Impedance matching occur
at 3.5GHz.
Figure 7: Electric field of Vivaldi antenna.
Figure 8: Gain of Vivaldi antenna.
Figure 9: (SWR).
Figure 10: Far field Radiation Pattern.
Figure 11: S-parameter.
Figure 12: 1D Impedance matching.
How to cite this article: Sunita R, Himanshu M, Silki B. Design and Performance Enhancement of Vivaldi Antenna. Res Dev Material Sci. 3(2). RDMS.000560.
2018. DOI: 10.31031/RDMS.2018.03.000560
Research & Development in Material Science
246
Res Dev Material Sci
Conclusion
The proposed Vivaldi antenna is simulated using the COMSOL.
The proposed antenna is low- profile and uses low cost FR4
substrate. Here the geometry is not restricted and it takes a shape
such that the objective of maximum gain and minimum S11 is
achieved. The designed antenna can be design frequency from
2 to 6.5GHz. This antenna is showing good impedance matching
performance at a frequency of 3.5GHz. The proposed antenna is
giving high electric field of 64. Low reflection losses are -24 and
gain of antenna is7.95db. The proposed antenna is low-profile and
uses low-cost FR-4 substrate. To validate the simulation results, the
antenna would be fabricated and tested in near future.
References
1.	 Rajveer D, Gurkiran D (2016) Vivaldi antenna simulation on defining
parameters, Parametric study and results. IJCTA 9(11): 5129-5138.
2.	 Matthias J, Ammann MJ, Mcevoy P (2008) UWB vivaldi antenna based on
a spline geometry with frequency band-notch. IEEE.
3.	 Yang Y, Wang Y, Fathy AE (2008) Design of compact vivaldi antenna
arrays for UWB see through wall applications. Electromagnetics
Research 82: 401-418.
4.	 Han X, Juan L, Changjuan C, Lin A (2012) UWB dual polarized vivaldi
antenna with high gain. IEEE.
5.	 Kerarti DZ, Marouf FZ, Meriah SM (2012) New tapered slot vivaldi
antenna for UWB applications. 24th
ICM.
6.	 Debdeep S, Vaibhav S (2013) SRR-loaded antipodal vivaldi antenna
for UWB applications with tunable notch function. Proceedings of The
International Symposium On Electromagnetic Theory. IEEE.
7.	 Chittajit S (2014) Some parametric studies on vivaldi antenna.
International Jornal of U-And -E Service Science and Technology 7(4):
323-328.
8.	 Anu RGS, Santhosh K (2014) Tapered slotted vivaldi antenna design
using fourier series approach for UWB applications. ICCSC.
9.	 Pandey GK, Singh HS, Bharti PK, Pandey A, Meshram MK (2015) High
gain vivaldi antenna for radar and microwave imaging applications.
International Journal of Signal Processing Systems 3(1): 35-39.
10.	Kalyani PD, Narlawar MS (2015) Design of novel vivaldi antenna for
cognitive radio application in ultra wide band 3(3).
11.	Osama MD, Tamer GA, Ashraf SM, Hadia MEH (2016) A novel UWB
vivaldi antenna array for radar applications. International Journal Of
Scientific & Engineering Research 7(5).
12.	Ying L, Ai-Xin C (2008) Design and application of vivaldi antenna array.
IEEE.

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Design and Performance Enhancement of Vivaldi Antenna - Crimson Publishers

  • 1. Research & Development in Material Science 242 Res Dev Material Sci 242 Introduction The Vivaldi antenna is a special kind of tapered slot antenna (TSA), having an exponentially tapered slot profile. It is first recognized by Gibson in 1979 [1-3]. It is useful for wide-band applications [4]. This research focused mainly on miniature antennas with a low losses and high gain. The aim of this research is to compute the far-field pattern and to compute the impedance matching of the structure [5,6] (Figure 1). Sunita Rani, Himanshu Monga* and Silki Baghla Department of ECE, JCDM College of Engineering, India *Corresponding author: Himanshu Monga, Department of ECE, Sirsa, India Submission: December 04, 2017; Published: January 25, 2018 Design and Performance Enhancement of Vivaldi Antenna Copyright © All rights are reserved by Himanshu Monga. Abstract In this paper, a computer aided design of Vivaldi Antenna is developed which is used to study the effect of different parameters such as rate of opening of exponential slot and size of the radius of circular slot of the Vivaldi Antenna. The proposed design resulted in enhancement of gain and reduction in reflection losses. COMSOL Multi physics simulator is used to design the proposed Vivaldi antenna. Keywords: Vivaldi Antenna; COMSOL Multiphysics; Copper Plate (FR4, 3.38 dielectric value) Figure 1: Vivaldi antenna structure. The proposed Vivaldi antennas consist of a micro strip feed line, micro strip line to slot line transition, and the radiating structure. Radiating structure is exponential tapered and the radiation takes place along the axis of the tapering [7-9] This antenna comprises of three different types of slot lines which are: a. The circular slot which is used to realize the impedance matching of the micro strip transmission line. b. The rectangular slot which is used to couple the electromagnetic wave from the micro strip transmission line. c. The exponential tapered slot which is used. In this Vivaldi antenna model, the tapered slot is patterned with a prefect electric conductor (PEC) ground plane the top of the Short Communication Research & Development in Material Science C CRIMSON PUBLISHERS Wings to the Research ISSN: 2576-8840
  • 2. How to cite this article: Sunita R, Himanshu M, Silki B. Design and Performance Enhancement of Vivaldi Antenna. Res Dev Material Sci. 3(2). RDMS.000560. 2018. DOI: 10.31031/RDMS.2018.03.000560 243 Res Dev Material Sci Research & Development in Material Science dielectric substrate. One end of the slot is open to the air and other end is finished with a circular slot. On the bottom of the substrate, the shorted 50Ohm micro strip feed line is modeled PEC surface. The entire molding domain is bounded by perfectly matched layer (PEC) which act like an chamber absorbing all radiated energy. Related Work Dhawan [1] Presented the design and detailed results of the Vivaldi Antenna with the selection of FR4(2.33) substrate material. This antenna is showing remarkable performance at a frequency of 7.5GHz and VSWR equal to-24.5dB with high directivity and narrow beam width. Ying [3] proposed one design that starts from a single balanced Vivaldi antenna unit, designs and analyses the electromagnetic characteristics of balanced Vivaldi antenna array. Then get a high-gain more than 35dB successfully by a parabolic antenna with the feed of 4 × 3 × 3 Vivaldi array. ANU [8] designed an antenna which used in the band from 2.1GHz to 9.2GHz with a fractional bandwidth of 125.66%. Corresponding to the design frequency of 2.8GHz a peak gain of 6.122dB and minimum S11 of -28.5dB is achieved [10-12]. Design Parameters of Proposed Antenna General parameters that are used during the design of Vivaldi are given in Table 1. Table 1: Design parameters. Name Expression Value Description W-slot 0.5 [mm] 5.000E-4 m Slot width Thickness 60 [mil] 0.0015240 m Substrate thickness F-max 6.0 [GHz] 6.0000E9 Hz Maximum Frequency in sweep F-min 2.0 [GHz] 2.0000E9Hz Minimum frequency in sweep F0 F-max 6.5000E9 Hz Current frequency in sweep Length 110 [mm] 011000 m Length of antenna Radius 10 [mm] 0.012000 m Radius of circular slot Width 80 [mm] 0.080000 m Width of antenna Dielectric 3.38 33800 Dielectric constant of substrate Design Procedure The proposed VIVALDI antenna is designed using COMSOL simulate with following step: a. Select the dimensions. b. The Vivaldi antenna is realized on a thin dielectric substrate. The Vivaldi block with the dimensions given in Table 1 is drawn on substrate FR4. The length of the Vivaldi antenna is 110mm, thickness is 1.5mm and breadth is 80mm Figure 2. Figure 2: Substrate. c. In the next step, feed line is selected. In this work the feed line with the line width=3.2, Depth=0+w_slot/2, Height =thickness breadth of 5mm and length 16mm is drawn. Shown in Figure 3. Figure 3: Feed line.
  • 3. How to cite this article: Sunita R, Himanshu M, Silki B. Design and Performance Enhancement of Vivaldi Antenna. Res Dev Material Sci. 3(2). RDMS.000560. 2018. DOI: 10.31031/RDMS.2018.03.000560 Research & Development in Material Science 244 Res Dev Material Sci d. Under a plane geometry node we define and create the geometry sequence for a work plane. The plane geometry node also contains some settings for the visualization of the work plane’s geometry. Plane geometry for the proposed antenna with the radius of 10mm is show in Figure 4. e. Apply electromagnetic wave in frequency domain and the antenna is made up of FR4 material with electrical permeability Figure 4-6. Figure 4: Plane geometry. Figure 5: Electromagnetic waves, frequency domain. Figure 6: Mesh. f. In this step, the antenna will be divided into small part. A mesh imported into COMSOL can be used to construct geometry. Discussion & Results The proposed antenna is analyzed with variation in radius and it is found that at radius of 10mm. The designed antenna provides maximum electric field of 64 as show in Figure 7. When
  • 4. How to cite this article: Sunita R, Himanshu M, Silki B. Design and Performance Enhancement of Vivaldi Antenna. Res Dev Material Sci. 3(2). RDMS.000560. 2018. DOI: 10.31031/RDMS.2018.03.000560 245 Res Dev Material Sci Research & Development in Material Science then electric field of Vivaldi antenna is 64 the designed antenna promotes the gain from 7.95dB in the desired frequency band (2 to 6.5GHz) as shown in Figure 8. The improved antenna gain can be used for applications like microwave imaging and radars. The result of our simulation can be seen in the form of SWR plot. According to our result SWR parameter is minimum 1.14 at 3.5GHz as shown in Figure 9 & Figure 10 Show the Far field radiation pattern for FR4, beginning frequency is 2GHz and 6.5GHz that is the finish frequency. In this far field, radiation pattern diagram highest output frequency at 4.5GHz. With the selection of feed purpose employed in this model, the S11 parameter is minimum at 3.5GHz as shown in Figure 11 & Figure 12 shows a good Impedance matching occur at 3.5GHz. Figure 7: Electric field of Vivaldi antenna. Figure 8: Gain of Vivaldi antenna. Figure 9: (SWR). Figure 10: Far field Radiation Pattern. Figure 11: S-parameter. Figure 12: 1D Impedance matching.
  • 5. How to cite this article: Sunita R, Himanshu M, Silki B. Design and Performance Enhancement of Vivaldi Antenna. Res Dev Material Sci. 3(2). RDMS.000560. 2018. DOI: 10.31031/RDMS.2018.03.000560 Research & Development in Material Science 246 Res Dev Material Sci Conclusion The proposed Vivaldi antenna is simulated using the COMSOL. The proposed antenna is low- profile and uses low cost FR4 substrate. Here the geometry is not restricted and it takes a shape such that the objective of maximum gain and minimum S11 is achieved. The designed antenna can be design frequency from 2 to 6.5GHz. This antenna is showing good impedance matching performance at a frequency of 3.5GHz. The proposed antenna is giving high electric field of 64. Low reflection losses are -24 and gain of antenna is7.95db. The proposed antenna is low-profile and uses low-cost FR-4 substrate. To validate the simulation results, the antenna would be fabricated and tested in near future. References 1. Rajveer D, Gurkiran D (2016) Vivaldi antenna simulation on defining parameters, Parametric study and results. IJCTA 9(11): 5129-5138. 2. Matthias J, Ammann MJ, Mcevoy P (2008) UWB vivaldi antenna based on a spline geometry with frequency band-notch. IEEE. 3. Yang Y, Wang Y, Fathy AE (2008) Design of compact vivaldi antenna arrays for UWB see through wall applications. Electromagnetics Research 82: 401-418. 4. Han X, Juan L, Changjuan C, Lin A (2012) UWB dual polarized vivaldi antenna with high gain. IEEE. 5. Kerarti DZ, Marouf FZ, Meriah SM (2012) New tapered slot vivaldi antenna for UWB applications. 24th ICM. 6. Debdeep S, Vaibhav S (2013) SRR-loaded antipodal vivaldi antenna for UWB applications with tunable notch function. Proceedings of The International Symposium On Electromagnetic Theory. IEEE. 7. Chittajit S (2014) Some parametric studies on vivaldi antenna. International Jornal of U-And -E Service Science and Technology 7(4): 323-328. 8. Anu RGS, Santhosh K (2014) Tapered slotted vivaldi antenna design using fourier series approach for UWB applications. ICCSC. 9. Pandey GK, Singh HS, Bharti PK, Pandey A, Meshram MK (2015) High gain vivaldi antenna for radar and microwave imaging applications. International Journal of Signal Processing Systems 3(1): 35-39. 10. Kalyani PD, Narlawar MS (2015) Design of novel vivaldi antenna for cognitive radio application in ultra wide band 3(3). 11. Osama MD, Tamer GA, Ashraf SM, Hadia MEH (2016) A novel UWB vivaldi antenna array for radar applications. International Journal Of Scientific & Engineering Research 7(5). 12. Ying L, Ai-Xin C (2008) Design and application of vivaldi antenna array. IEEE.