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International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019
DOI: 10.5121/ijwmn.2019.11204 39
WIDTH FEEDING STRIPLINE OPTIMISE OF CURVED
MICROSTRIPLINE ARRAY VARIANS ANTENNA IN
MULTIBAND FREQUENCY FOR RADAR
COMMUNICATIONS
Putu Artawan1
, Josaphat T. Sri Sumantyo2
, Mashuri1
and Yono Hadi Pramono1
1
Physics Department, Faculty of Natural Sciences, Institut Teknologi Sepuluh Nopember
(ITS), Surabaya, Indonesia
2
Josaphat Microwave Remote Sensing Laboratory, Center for Environmental Remote
Sensing (CEReS) Chiba University, 1-33 Yayoi-cho, Inage-ku, Chiba 263-8522-Japan
ABSTRACT
This study proposed to design of curved microstripline array antenna with more optimal characteristics
parametric through optimise in width feeding stripline and its application for radar communications.
Numeric analysis with an empirical formula in curved microstripline array antenna supports the counting in
relation to the characteristics antenna that is optimally applied in communications. The simulations was
created by using CST software. The result of simulation is to indicate Voltage Standing Wave Ratio (VSWR),
Reflection coefficient, Return Loss and Gain with Vertical Linear Polarization. The optimise of curved
microstripline array varians with the varians array and optimise varians in width of the feeding stripline.
Based on this simulated result, curved microstripline array varians antenna is potential to developed antenna
in radar communication in multiband frequency.
KEYWORDS
Simulation, Curved Microstripline, Multi Band Frequency, Radar Communication
1. INTRODUCTION
To design and analyze the shape and size of the antenna required special knowledge regarding the
electromagnetic field theory. Electromagnetic fields generated depend on the distance of the source
access and terrain [2]. The further course of electromagnetic fields produced less meaning in the
spread process electromagnetic waves from the transmitter to the receiver experiencing attenuation
(weakening) signals. Therefore, the required antenna design with specific dimensions that have a
high gain value and high directivity with return loss is very small [3]. Various studies have been
conducted on microstrip antenna [1,7,8,9,12,17]. In this research proposed new type of antenna that
will be designed to have the characteristics in question are Curved Microstripline Array Antenna
Design. This antenna is an antenna type Microstrip with the characteristics of a thin cross section,
the mass that is lightweight, easy to make, can be easily integrated with Microwave Integrated
Circuits (MICs) and can be made to multifrequency [4,5,6]. In this research, Novel curved
microstripline array antenna design and its optimise is propose to develope in Multiband frequency
for radar communications. The optimise in width feeding stripline will be done to get optimal result
in antenna parametric that as a good performance indicator in multiband frequencies for radar
communication application. The proposed Novel curved microstripline array antenna is afford to
International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019
40
operate in Multiband frequency. The target of Novel curved microstripline array antenna is in
multiband frequency, reflection coefficient less than –10dB, Voltage Standing Wave Ratio
(VSWR) less than 2, gain more than 5dB, respectively.
2. EMPIRICAL ANALYSIS AND DESIGN
The first calculating is to find the total electricity permittivity (εrtot) using the capacitor equation:
21tot c
1
c
1
c
1
+=
2211 /
1
/
1
/
1
21
dAdAtotdA rorototro 
+=
where εr1 isεr for air (εr1 = 1), εr2 isεr for substrate (εr FR4 = 4.3), 1d thick of substrate and 2d distance
of substrate to the reflector, with dtot is d1+d2.
And then using the following equation:
555,0
w
h
101
2
1
2
1
−






+
−
+
+
= rr
eff


To calculate the effective permittivity electricity ( eff ). Where εr is the same with εrtot, h is dtot and
w is the various wide for patch and stripline side.
The following equation is to know the maximum dimension in the patch side (w1):
f =
2c
3w√ 𝜀 𝑟
𝑤1 =
2c
3√ 𝜀 𝑟 f
where c is lightspeed in air, εr is electricity permittivity and f is frequency.
And to calculate the effective width stripline side (w2,3), using the following figure:
1
2
.f2
1
W
0
2,3
+
=
roZ 
Where f is frequency, o is permeability constant and Zo is characteristic impedance.
The calculation wavelength of the substrate ( g ), using the following equation:
𝜆𝑔 =
𝜆
√ 𝜀 𝑒𝑓𝑓
From the analysis above we find to fix the parameter of antenna fabrication.
The following figure is the Curved Microstripline Antenna Design in array varians.
International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019
41
Figure 4. (a) Curved Microstripline 2x2 Array Antenna Design
(b) Dimension of Curved Microstripline 2x2 Array Antenna Design
Figure 5. Model 1 and 2 width feeding stripline varians
(Curved Microstripline 2x4 Array Antenna Design)
Figure 6. Model 1 and 2 width feeding stripline varians
(Curved Microstripline 4x4 Array Antenna Design)
W1
International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019
42
3. RESULT AND DISCUSSION
The simulation result of Curved Microstripline 2x2 Array Antenna Design:
Figure 7. Model 1 and 2 width feeding stripline varians
(S11 Parameter Simulation)
Figure 8. Model 1 and 2 width feeding stripline varians
(VSWR Parameter Simulation)
International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019
43
Figure 9. Model 1 and 2 width feeding stripline varians
(Radiation Pattern Parameter Simulation)
The result indicate that the Curved Microstripline 2x2 Array Antenna Design work in multi band
frequency (f=2GHz, f=4.5GHz, f=5.5GHz, f=8GHz, f=9.8GHz) with approximately VSWR < 2,
Return Loss < -10dB and 5.27dB Gain in Omnidirectional radiation pattern.
The simulation result of Curved Microstripline 2x4 Array Antenna Design:
Figure 10. Model 1 and 2 width feeding stripline varians(S11 Parameter Simulation)
Figure 11. Model 1 and 2 width feeding stripline varians(VSWR Parameter Simulation)
Model 1
0
5000
1.00
1.50
2.01
2.51
3.02
3.52
4.02
4.53
5.03
5.54
6.04
6.54
7.05
7.55
8.06
8.56
9.06
9.57
VSWR
Frekuensi (GHz)
VSWR
Model 1
Model 2
International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019
44
Figure 12. Model 1 and 2 width feeding stripline varians
(Radiation Pattern Parameter Simulation)
The result indicate that the Curved Microstripline 2x4 Array Antenna Design work in multi band
frequency (f=4.6GHz, f=5.4GHz, f=7.2GHz, f=9.8GHz) with approximately VSWR < 2, Return
Loss < -10dB and 4.50dB Gain in Omnidirectional radiation pattern.
The simulation result of Curved Microstripline 4x4 Array Antenna Design:
Figure 13. Model 1 and 2 width feeding stripline varians
(S11 Parameter Simulation)
International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019
45
Figure 14. Model 1 and 2 width feeding stripline varians
(VSWR Parameter Simulation)
Figure 15. Model 1 and 2 width feeding stripline varians
(Radiation Pattern Parameter Simulation)
The result indicate that the Curved Microstripline 4x4 Array Antenna Design work in multi band
frequency (f=2.0GHz, f=3.9GHz, f=4.5GHz, f=4.9GHz, f=5.8GHz, f=6.6GHz, f=7.7GHz,
f=8.9GHz) with approximately VSWR < 2, Return Loss < -10dB and 6.14dB Gain in
Omnidirectional radiation pattern.
4. CONCLUSION
Width feeding stripline optimise of Curved Microstripline Array Varians Antenna in multiband
frequency for radar communications has been presented in this paper. In general, the result was
indicate that Curved Microstripline Array Varians Antenna design work in multiband frequency
and its can be operated in radar communication application recently. The satisfy indicator parameter
characteristic are obtain in term of reflection coeficient, voltage standing wave ratio, return loss,
axial ratio and radiation pattern. But, the gain in this antenna still small less than 10dB. This gain
result influenced by the dimension in stripline feeding and need more analysis increasing the gain.
Based on this result, the proposed Curved Microstripline Array Varians Antenna can be
implemented in Radar communication systems.
International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019
46
5. ACKNOWLEDGMENT
The authors would like to thank the Indonesian Ministry of Research, Technology and Higher
Education through LPDP and PKPI (Sandwich-like) scholarships, Center for Environmental
Remote Sensing (CEReS), Josaphat Tetuko Sri Sumantyo (JMRSL Chiba University), Promotor
Yono Hadi Pramono and Mashuri (Physics Department, ITS Surabaya).
REFERENCES
[1] Balanis, C.A. Antena Theory Analysis and Design, Second Edition, John Wiley and Sons, NewYork,
1997.
[2] Edward, Terry. Foundation For Microstrip Circuit Design. Knaresborough England, 1991.
[3] Shafai. Microstrip Antena Design Handbook, Profesor University Of Manitoba, Wimmipeg, Canada,
2001.
[4] ]Kraus, John, D. Electromagnetics, Third Edition, McGraw-Hill, New York, 1984.
[5] Hund, E. Microwave Communications, Component and Circuit, McGraw Hill, New York, 1989.
[6] Hadi Pramono,Yono. Prototipe Antenna Bi-Mikrostrip tapered patch Dengan Dua Arah Pola Radiasi
Dan Satu Feeding Monopole Beroperasi Pada Freq.2,4 GHz. Prosiding T. Informatika, UPN.
Yogyakarta, 2009.
[7] Hidayah, Ifa. Desain dan Fabrikasi Antena Bi-Mikrostrip tapered patch dengan Dua Arah Radiasi dan
Satu Feeding Monopole Untuk Komunikasi Wi-fi. Tesis Magister. Institut Tekologi Sepuluh
Nopember. Surabaya, 2009.
[8] Risfaula, Erna. Antena Mikrostrip Panel Berisi 5 Larik Dipole dengan Feedline Koaksial Waveguide
untuk Komunikasi 2,4 GHz. Program Keahlian Optoelektronika Jurusan fisika FMIPA-ITS: Surabaya,
2011.
[9] S. Gao, Q. Luo, F. Zhu, Circularly Polarized Antenna, John Wiley & Sons, Ltd, 2014.
[10] S. Murugan, V. Rajamani, “Study of broadband circularly polarised microstrip antenna” Science
Engineering and Management Research (ICSEMR), 2014 International Conference on. IEEE, 2014.
[11] Haider Raad, “An UWB Antenna Array for Flexible IoT Wireless System,” Progress In
Electromagnetics Research, Vol. 162, 109-121, 2018.
[12] Kurniawan Farohaji, Sri Sumantyo, J. T, Gao Steven, Ito Koichi, Edi Santosa C. “Square-shaped feeding
truncated circularly polarised slot antenna”. IET Microwaves, Antenna & Propagation Journals. ISSN
1751-8725, 2018.
[13] Edi Santosa C, Sri Sumantyo, J.T, Yam Chua Ming, Urata Katia, Ito Koichi, Gao Steven. “Subarray
Design for C-Band Circularly-Polarized Synthetic Aperture Radar Antenna Onboard Airborne,”
Progress In Electromagnetics Research, Vol. 163, 107-117, 2018.
[14] Xu Mao-Chun, Gao Steven, Wang Yi, Sri Sumantyo, J.T. “Compact Broadband Dual-Sense Circularly
Polarized Microstrip Antenna/Array With Enhanced Isolation”. IEEE Transactions on Antennas And
Propagation, Vol 65, No.12, 2017.
International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019
47
[15] Luo Qi, Gao Steven, Sobhy Mohammed, Sri Sumantyo, J.T, Li Jianzhou, Wei Gao, Xu Jiadong, Wu
Changying. “Dual Circularly Polarised Equilateral Triangular Patch Array”. IEEE Transactions on
Antennas And Propagation, Vol 64, No.6, 2016.
[16] Kumar Dwivedi M, Srivastava Pragati. “Microstrip Patch Array Antenna for X Band Application”.
Antenna Test and Measurement Society (ATMS India-16), 01-03 Feb, 2016.
Authors
The author is a lecturer in Physics Departement, Math and Science Faculty, Ganesha
University of Education since 2006. He was graduated in IKIP N Singaraja (now as
UNDIKSHA) and got his master degree in ITS Surabaya. The subjects he had taught; Basic
Physics 1, Basic Physics 2, Calculus 1, Calculus 2, Physics Laboratory 1, Physics
Laboratory 2, Mathematical Physics 1, Mathematical Physics 2, Mechanical Physics,
Electromagnetic, Optic and Wave, Statistical Physics and Solid Physics in regular class and
RKBI (preparing to International Class). The author also advises schools/students in physics
olympiads preparation. Besides teaching the author is activelly involved in some researches.
Now, this the author as a doctoral student in Physics Departement, Faculty of Science, ITS Surabaya
Indonesia.

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WIDTH FEEDING STRIPLINE OPTIMISE OF CURVED MICROSTRIPLINE ARRAY VARIANS ANTENNA IN MULTIBAND FREQUENCY FOR RADAR COMMUNICATIONS

  • 1. International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019 DOI: 10.5121/ijwmn.2019.11204 39 WIDTH FEEDING STRIPLINE OPTIMISE OF CURVED MICROSTRIPLINE ARRAY VARIANS ANTENNA IN MULTIBAND FREQUENCY FOR RADAR COMMUNICATIONS Putu Artawan1 , Josaphat T. Sri Sumantyo2 , Mashuri1 and Yono Hadi Pramono1 1 Physics Department, Faculty of Natural Sciences, Institut Teknologi Sepuluh Nopember (ITS), Surabaya, Indonesia 2 Josaphat Microwave Remote Sensing Laboratory, Center for Environmental Remote Sensing (CEReS) Chiba University, 1-33 Yayoi-cho, Inage-ku, Chiba 263-8522-Japan ABSTRACT This study proposed to design of curved microstripline array antenna with more optimal characteristics parametric through optimise in width feeding stripline and its application for radar communications. Numeric analysis with an empirical formula in curved microstripline array antenna supports the counting in relation to the characteristics antenna that is optimally applied in communications. The simulations was created by using CST software. The result of simulation is to indicate Voltage Standing Wave Ratio (VSWR), Reflection coefficient, Return Loss and Gain with Vertical Linear Polarization. The optimise of curved microstripline array varians with the varians array and optimise varians in width of the feeding stripline. Based on this simulated result, curved microstripline array varians antenna is potential to developed antenna in radar communication in multiband frequency. KEYWORDS Simulation, Curved Microstripline, Multi Band Frequency, Radar Communication 1. INTRODUCTION To design and analyze the shape and size of the antenna required special knowledge regarding the electromagnetic field theory. Electromagnetic fields generated depend on the distance of the source access and terrain [2]. The further course of electromagnetic fields produced less meaning in the spread process electromagnetic waves from the transmitter to the receiver experiencing attenuation (weakening) signals. Therefore, the required antenna design with specific dimensions that have a high gain value and high directivity with return loss is very small [3]. Various studies have been conducted on microstrip antenna [1,7,8,9,12,17]. In this research proposed new type of antenna that will be designed to have the characteristics in question are Curved Microstripline Array Antenna Design. This antenna is an antenna type Microstrip with the characteristics of a thin cross section, the mass that is lightweight, easy to make, can be easily integrated with Microwave Integrated Circuits (MICs) and can be made to multifrequency [4,5,6]. In this research, Novel curved microstripline array antenna design and its optimise is propose to develope in Multiband frequency for radar communications. The optimise in width feeding stripline will be done to get optimal result in antenna parametric that as a good performance indicator in multiband frequencies for radar communication application. The proposed Novel curved microstripline array antenna is afford to
  • 2. International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019 40 operate in Multiband frequency. The target of Novel curved microstripline array antenna is in multiband frequency, reflection coefficient less than –10dB, Voltage Standing Wave Ratio (VSWR) less than 2, gain more than 5dB, respectively. 2. EMPIRICAL ANALYSIS AND DESIGN The first calculating is to find the total electricity permittivity (εrtot) using the capacitor equation: 21tot c 1 c 1 c 1 += 2211 / 1 / 1 / 1 21 dAdAtotdA rorototro  += where εr1 isεr for air (εr1 = 1), εr2 isεr for substrate (εr FR4 = 4.3), 1d thick of substrate and 2d distance of substrate to the reflector, with dtot is d1+d2. And then using the following equation: 555,0 w h 101 2 1 2 1 −       + − + + = rr eff   To calculate the effective permittivity electricity ( eff ). Where εr is the same with εrtot, h is dtot and w is the various wide for patch and stripline side. The following equation is to know the maximum dimension in the patch side (w1): f = 2c 3w√ 𝜀 𝑟 𝑤1 = 2c 3√ 𝜀 𝑟 f where c is lightspeed in air, εr is electricity permittivity and f is frequency. And to calculate the effective width stripline side (w2,3), using the following figure: 1 2 .f2 1 W 0 2,3 + = roZ  Where f is frequency, o is permeability constant and Zo is characteristic impedance. The calculation wavelength of the substrate ( g ), using the following equation: 𝜆𝑔 = 𝜆 √ 𝜀 𝑒𝑓𝑓 From the analysis above we find to fix the parameter of antenna fabrication. The following figure is the Curved Microstripline Antenna Design in array varians.
  • 3. International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019 41 Figure 4. (a) Curved Microstripline 2x2 Array Antenna Design (b) Dimension of Curved Microstripline 2x2 Array Antenna Design Figure 5. Model 1 and 2 width feeding stripline varians (Curved Microstripline 2x4 Array Antenna Design) Figure 6. Model 1 and 2 width feeding stripline varians (Curved Microstripline 4x4 Array Antenna Design) W1
  • 4. International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019 42 3. RESULT AND DISCUSSION The simulation result of Curved Microstripline 2x2 Array Antenna Design: Figure 7. Model 1 and 2 width feeding stripline varians (S11 Parameter Simulation) Figure 8. Model 1 and 2 width feeding stripline varians (VSWR Parameter Simulation)
  • 5. International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019 43 Figure 9. Model 1 and 2 width feeding stripline varians (Radiation Pattern Parameter Simulation) The result indicate that the Curved Microstripline 2x2 Array Antenna Design work in multi band frequency (f=2GHz, f=4.5GHz, f=5.5GHz, f=8GHz, f=9.8GHz) with approximately VSWR < 2, Return Loss < -10dB and 5.27dB Gain in Omnidirectional radiation pattern. The simulation result of Curved Microstripline 2x4 Array Antenna Design: Figure 10. Model 1 and 2 width feeding stripline varians(S11 Parameter Simulation) Figure 11. Model 1 and 2 width feeding stripline varians(VSWR Parameter Simulation) Model 1 0 5000 1.00 1.50 2.01 2.51 3.02 3.52 4.02 4.53 5.03 5.54 6.04 6.54 7.05 7.55 8.06 8.56 9.06 9.57 VSWR Frekuensi (GHz) VSWR Model 1 Model 2
  • 6. International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019 44 Figure 12. Model 1 and 2 width feeding stripline varians (Radiation Pattern Parameter Simulation) The result indicate that the Curved Microstripline 2x4 Array Antenna Design work in multi band frequency (f=4.6GHz, f=5.4GHz, f=7.2GHz, f=9.8GHz) with approximately VSWR < 2, Return Loss < -10dB and 4.50dB Gain in Omnidirectional radiation pattern. The simulation result of Curved Microstripline 4x4 Array Antenna Design: Figure 13. Model 1 and 2 width feeding stripline varians (S11 Parameter Simulation)
  • 7. International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019 45 Figure 14. Model 1 and 2 width feeding stripline varians (VSWR Parameter Simulation) Figure 15. Model 1 and 2 width feeding stripline varians (Radiation Pattern Parameter Simulation) The result indicate that the Curved Microstripline 4x4 Array Antenna Design work in multi band frequency (f=2.0GHz, f=3.9GHz, f=4.5GHz, f=4.9GHz, f=5.8GHz, f=6.6GHz, f=7.7GHz, f=8.9GHz) with approximately VSWR < 2, Return Loss < -10dB and 6.14dB Gain in Omnidirectional radiation pattern. 4. CONCLUSION Width feeding stripline optimise of Curved Microstripline Array Varians Antenna in multiband frequency for radar communications has been presented in this paper. In general, the result was indicate that Curved Microstripline Array Varians Antenna design work in multiband frequency and its can be operated in radar communication application recently. The satisfy indicator parameter characteristic are obtain in term of reflection coeficient, voltage standing wave ratio, return loss, axial ratio and radiation pattern. But, the gain in this antenna still small less than 10dB. This gain result influenced by the dimension in stripline feeding and need more analysis increasing the gain. Based on this result, the proposed Curved Microstripline Array Varians Antenna can be implemented in Radar communication systems.
  • 8. International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019 46 5. ACKNOWLEDGMENT The authors would like to thank the Indonesian Ministry of Research, Technology and Higher Education through LPDP and PKPI (Sandwich-like) scholarships, Center for Environmental Remote Sensing (CEReS), Josaphat Tetuko Sri Sumantyo (JMRSL Chiba University), Promotor Yono Hadi Pramono and Mashuri (Physics Department, ITS Surabaya). REFERENCES [1] Balanis, C.A. Antena Theory Analysis and Design, Second Edition, John Wiley and Sons, NewYork, 1997. [2] Edward, Terry. Foundation For Microstrip Circuit Design. Knaresborough England, 1991. [3] Shafai. Microstrip Antena Design Handbook, Profesor University Of Manitoba, Wimmipeg, Canada, 2001. [4] ]Kraus, John, D. Electromagnetics, Third Edition, McGraw-Hill, New York, 1984. [5] Hund, E. Microwave Communications, Component and Circuit, McGraw Hill, New York, 1989. [6] Hadi Pramono,Yono. Prototipe Antenna Bi-Mikrostrip tapered patch Dengan Dua Arah Pola Radiasi Dan Satu Feeding Monopole Beroperasi Pada Freq.2,4 GHz. Prosiding T. Informatika, UPN. Yogyakarta, 2009. [7] Hidayah, Ifa. Desain dan Fabrikasi Antena Bi-Mikrostrip tapered patch dengan Dua Arah Radiasi dan Satu Feeding Monopole Untuk Komunikasi Wi-fi. Tesis Magister. Institut Tekologi Sepuluh Nopember. Surabaya, 2009. [8] Risfaula, Erna. Antena Mikrostrip Panel Berisi 5 Larik Dipole dengan Feedline Koaksial Waveguide untuk Komunikasi 2,4 GHz. Program Keahlian Optoelektronika Jurusan fisika FMIPA-ITS: Surabaya, 2011. [9] S. Gao, Q. Luo, F. Zhu, Circularly Polarized Antenna, John Wiley & Sons, Ltd, 2014. [10] S. Murugan, V. Rajamani, “Study of broadband circularly polarised microstrip antenna” Science Engineering and Management Research (ICSEMR), 2014 International Conference on. IEEE, 2014. [11] Haider Raad, “An UWB Antenna Array for Flexible IoT Wireless System,” Progress In Electromagnetics Research, Vol. 162, 109-121, 2018. [12] Kurniawan Farohaji, Sri Sumantyo, J. T, Gao Steven, Ito Koichi, Edi Santosa C. “Square-shaped feeding truncated circularly polarised slot antenna”. IET Microwaves, Antenna & Propagation Journals. ISSN 1751-8725, 2018. [13] Edi Santosa C, Sri Sumantyo, J.T, Yam Chua Ming, Urata Katia, Ito Koichi, Gao Steven. “Subarray Design for C-Band Circularly-Polarized Synthetic Aperture Radar Antenna Onboard Airborne,” Progress In Electromagnetics Research, Vol. 163, 107-117, 2018. [14] Xu Mao-Chun, Gao Steven, Wang Yi, Sri Sumantyo, J.T. “Compact Broadband Dual-Sense Circularly Polarized Microstrip Antenna/Array With Enhanced Isolation”. IEEE Transactions on Antennas And Propagation, Vol 65, No.12, 2017.
  • 9. International Journal of Wireless & Mobile Networks (IJWMN) Vol. 11, No.2, April 2019 47 [15] Luo Qi, Gao Steven, Sobhy Mohammed, Sri Sumantyo, J.T, Li Jianzhou, Wei Gao, Xu Jiadong, Wu Changying. “Dual Circularly Polarised Equilateral Triangular Patch Array”. IEEE Transactions on Antennas And Propagation, Vol 64, No.6, 2016. [16] Kumar Dwivedi M, Srivastava Pragati. “Microstrip Patch Array Antenna for X Band Application”. Antenna Test and Measurement Society (ATMS India-16), 01-03 Feb, 2016. Authors The author is a lecturer in Physics Departement, Math and Science Faculty, Ganesha University of Education since 2006. He was graduated in IKIP N Singaraja (now as UNDIKSHA) and got his master degree in ITS Surabaya. The subjects he had taught; Basic Physics 1, Basic Physics 2, Calculus 1, Calculus 2, Physics Laboratory 1, Physics Laboratory 2, Mathematical Physics 1, Mathematical Physics 2, Mechanical Physics, Electromagnetic, Optic and Wave, Statistical Physics and Solid Physics in regular class and RKBI (preparing to International Class). The author also advises schools/students in physics olympiads preparation. Besides teaching the author is activelly involved in some researches. Now, this the author as a doctoral student in Physics Departement, Faculty of Science, ITS Surabaya Indonesia.