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IOSR Journal of Electronics and Communication Engineering (IOSR-JECE)
e-ISSN: 2278-2834,p- ISSN: 2278-8735.Volume 10, Issue 3, Ver. III (May - Jun.2015), PP 01-09
www.iosrjournals.org
DOI: 10.9790/2834-10330109 www.iosrjournals.org 1 | Page
Hybrid Zeroth-Order Resonance Patch Antenna with Improved
Half Power Beamwidth
Pearl Antonette Mendez1
, Deepthi Das Krishna2
1,2
(Department of Electronics & Communication, Rajagiri school of Engineering & Technology,
Ernakulam, Kerala, India)
Abstract: Antenna miniaturization is a critical issue in today’s wireless and communication systems.
Omnidirectional antennas are useful for applications in wireless communication however these antennas
radiate towards the broadside and antennas should protrude from ground for large radiation area. Several
techniques to reduce antenna size have been proposed in the recent years. One approach is Metamaterial
(MTM) based zeroth-order resonator (ZOR), ZOR antennas with the same physical size present better
performance if compared to other techniques. The conventional rectangular patch antenna cannot radiate omni-
directionally, despite of structural stability. Resonant frequencies of the conventional rectangular patch antenna
depend on width and length of patch, and height of substrate because of finite wavelength. ZOR antennas are
designed by using the ZOR mode- one of many attractive properties of the metamaterial antennas. The antenna
utilizes the zeroth-order resonance (ZOR) mode of the mushroom structure and the TM010 mode of the
conventional rectangular patch. If the directional radiation pattern of a TM010 mode and the omni-directional
radiation pattern of a ZOR mode are combined at the same frequency, it is expected that the total radiation
pattern would have the broader beamwidth.
Keywords: Beam width, Fringing, Metamaterials, Microstrip antenna, Rectangular Patch Antenna, Zeroth
order resonance (ZOR) antenna.
I. Introduction
A patch antenna (also known as a rectangular microstrip antenna) is a type of radio antenna with a low
profile, which can be mounted on a flat surface. It consists of a flat rectangular sheet or "patch" of metal,
mounted over a larger sheet of metal called a ground plane. The radiation mechanism arises from discontinuities
at each truncated edge of the microstrip transmission line.[2]
The radiation at the edges causes the antenna to act
slightly larger electrically than its physical dimensions, so in order for the antenna to be resonant, a length of
microstrip transmission line slightly shorter than one-half a wavelength at the frequency is used. The rectangular
patch antenna is approximately a one-half wavelength long section of rectangular microstrip transmission line.
When air is the antenna substrate, the length of the rectangular microstrip antenna is approximately one-half of a
free-space wavelength. As the antenna is loaded with a dielectric as its substrate, the length of the antenna
decreases as the relative dielectric constant of the substrate increases.
The microstrip patch antennas have been one of the most popular antennas in modern wireless
communication systems as they have several desirable attributes, such as a low-profile planar configuration, a
light weight, a simple design principle, a low fabrication cost, and so on [1], [2]. The conventional rectangular
patch antenna has a directional radiation pattern at the TM010 mode. It has a relatively narrow scanning range
and hence it is difficult for the antenna to maintain a stable performance in the changing environments or the
moving systems. This disadvantage created a need for an antenna with an enhanced beamwidth. For obtaining a
broad beamwidth, many antennas using the various techniques have been reported. For example, by using the
phase array patch structures [3], the multilayered structures [4]–[6], or the parasitic radiators [7], [8], it is
possible to design the patch antennas with a broad beamwidth. However, they have several limitations such as a
larger size, a difficult design, and a multi-layered structure.
II. Rectangular Patch Antenna
A patch antenna is usually constructed on a dielectric substrate, using the same materials and
lithography processes used to make printed circuit boards. The most commonly employed microstrip antenna is
a Rectangular patch. Dimensions of the patch are finite along the length and width and hence the fields at the
edges undergo fringing. Radiation in patch antenna is due to the fringing field between the periphery of the
patch and the ground plane which is a function of dimension of patch and substrate height. It increases with the
height of the substrate. But as the height increases, surface waves which are unwanted radiations also increase,
so an optimum value for substrate height should be chosen. Fringing makes the microstrip line look wider
electrically compared to its physical dimensions. Since some of the waves travel in the substrate and some in air,
an effective dielectric constant is introduces to account for fringing and the wave propagation in the line.
Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth
DOI: 10.9790/2834-10330109 www.iosrjournals.org 2 | Page
2.1 Rectangular Patch Antenna With Etched Hole
A rectangular patch antenna with an etched rectangular hole is shown in fig 1. The rectangular hole is
etched in the center of a patch [15]. In addition, a circular patch and a gap (gp)as a feeding structure are
employed. A coaxial probe (50 ohms ) is directly connected with the circular patch. Therefore, the excited
power is coupled to the rectangular patch through the circular patch. A TM010 mode can be generated in this
structure like a conventional rectangular patch antenna. The dimensions of the antenna are as follows: Width of
the substrate Ws=45mm, Length of the substrate Ls =40mm, width of the etched hole We =11mm, Length of the
etched hole=6mm, gp=0.2mm, height of the substrate hs=3.175mm, Width of the patch Wp=15mm, Length of the
patch Lp=10mm, permittivity=2.2 and δd = 0.0009.
Fig. 1. Geometry of the rectangular patch antenna with an etched rectangular hole.
III. Mushroom Antenna
Mushroom antennas are made up of metamaterials which are synthetic material with unusual refractive
properties, used for wireless systems. Their Optical and electromagnetic properties can be engineered by
changing the geometry of its unit cells. Each artificial unit responds to the radiation from the source. The
collective result is the material’s response to the electromagnetic wave that is broader than normal. It can step up
radiated power of an antenna, stores energy reradiates, behaves as if it was much more larger. It is an infinite
wavelength antenna where infinite wavelength occurs because the propagation constant is zero. Hence its
frequency does not depend on its physical length, but on the reactance provided by its unit cell.
A circular patch is directly connected with the coaxial probe, and a gap is inserted between the
mushroom patch and circular patch. Therefore, an excited power is coupled from the circular patch to the
mushroom patch. In general, the mushroom antenna has an infinite wavelength mode at specific non-zero
frequency called a ZOR mode. The resonance frequency of a ZOR mode is determined by the area of a patch,
the radius of a via, and the height of a mushroom antenna. The dimensions of the antenna are as follows: Width
of the substrate Ws=45mm, Length of the substrate Ls =40mm, width of the etched hole We=11mm, Length of
the etched hole=6mm, gp=0.2mm, height of the substrate hs=3.175mm, Width of the patch Wp=15mm, Length of
the patch Lp=10mm,ε=2.2 and δd = 0.0009.
IV. Hybrid ZOR Antenna
Fig 2: Hybrid ZOR antenna
Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth
DOI: 10.9790/2834-10330109 www.iosrjournals.org 3 | Page
To combine two modes at the same frequency, the structure where the mushroom ZOR antenna is
inserted in the etched pattern of a rectangular patch antenna, is designed. The antenna utilizes the zeroth-order
resonance (ZOR) mode [9], [10] of the mushroom structure and the TM010 mode of the conventional rectangular
patch .Therefore, the proposed antenna is composed of two radiators. This antenna will be called as a hybrid
ZOR antenna since it operates with the TM010 mode and the ZOR mode at the same frequency with a single
feed. First, the rectangular etched hole allows the patch antenna to have a lower resonance frequency of the
TM010 mode without changing the radiation pattern, the E-plane HPBW, and the size of an antenna. Second, the
mushroom ZOR antenna has the omni-directional pattern. If it is assumed that the resonance frequency of the
ZOR mode is the same as that of the TM010 mode and two modes are generated simultaneously, the directional
radiation pattern and the omni-directional pattern can be combined. It is expected that the total radiation pattern
would have the broader beamwidth. First, the etched rectangular hole is patterned on the center of the
rectangular patch and, then, the mushroom ZOR antenna is inserted inside the hole. At the ZOR mode, an
equivalent horizontal magnetic loop current is generated inside the mushroom structure, resulting in a low-
profile omni-directional radiation pattern [11]–[14].
This proposed antenna has structurally several advantages. First, the antenna needs only single-layered
substrate and maintains a planar configuration. Second, although the antenna has two radiators, a small size can
be achieved because the mushroom ZOR antenna is added inside the etched hole. Finally, it has a simple
structure. In order to excite the TM010 mode of an outer patch and the ZOR mode of an inner mushroom patch
simultaneously, a circular feeding patch is inserted between two patches. The circular patch is directly
connected to the coaxial probe. Thus, two radiators receive the incident power from the single feed. In addition,
two gaps of gp and gm are added between the circular patch and two radiators in order to independently control
the injected power to each antenna.
V. Figures And Tables
Fig 3: Rectangular patch antenna with etched hole width= 3mm
Fig 4: Resonant frequency of Rectangular patch antenna with etched hole width= 3mm
Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth
DOI: 10.9790/2834-10330109 www.iosrjournals.org 4 | Page
Fig 5: Rectangular patch antenna with etched hole width=11mm
Fig 6: Resonant frequency of Rectangular patch antenna with etched hole width= 3mm
Fig 7: Radiation efficiency of Rectangular patch antenna
Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth
DOI: 10.9790/2834-10330109 www.iosrjournals.org 5 | Page
Fig 8: Resonant frequency of Rectangular patch antenna with etched hole width= 5mm
Fig 9: Resonant frequency of Rectangular patch antenna with etched hole width= 7mm
Fig 10: Resonant frequency of Rectangular patch antenna with etched hole width= 9mm
Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth
DOI: 10.9790/2834-10330109 www.iosrjournals.org 6 | Page
Fig 11: Mushroom antenna
Fig 12: Resonant frequency of Mushroom antenna
Fig 13: HPBW of Mushroom Antenna
Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth
DOI: 10.9790/2834-10330109 www.iosrjournals.org 7 | Page
Fig 14: Hybrid ZOR antenna
Fig 15: Resonant frequency of hybrid ZOR antenna
Fig 16: Radiation efficiency of hybrid antenna
Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth
DOI: 10.9790/2834-10330109 www.iosrjournals.org 8 | Page
Fig 17: HPBW of hybrid ZOR antenna
Table 1: Effect of Resonant frequency on etched hole width for rectangular patch antenna with etched hole
Sl no Etched hole width (mm) Resonant frequency (GHz)
1 3 5.2
2 5 5.05
3 7 4.8
4 9 4.49
5 11 4.13
Table 2: Comparison of the parameters of the proposed antenna with Rectangular Patch
Parameters Rectangular Patch Mushroom antenna Hybrid ZOR antenna
Resonant frequency 4.22 GHz 13.9 GHz 4.31 GHz
Half power beam width 24.8° 117.5° 99.7°
Radiation efficiency 75% 20.14% 69%
Radiated power 0.23 W 0.0053 W 0.056 W
VI. Summary Of Results
Rectangular patch antenna has very low HPBW and hence is not ideal in moving environments because
of its very low scanning range. By employing the rectangular etched hole, the resonance frequency of the patch
antenna is down-shifted without changing the HPBW and the size of the antenna. The E-plane HPBW is
broadened compared with that of the conventional patch antenna. The proposed antenna has not only the broader
E-plane HPBW but also the smaller size than the conventional rectangular patch antenna. Even though
mushroom antenna has the maximum HPBW, it has very low radiation efficiency and cannot be used. So when
both antennas are combined, the E Plane beamwidth as well as radiation efficiency is increased.
VII. Conclusion
A hybrid ZOR patch antenna having the broad E-plane beamwidth is designed and simulated. In order
to obtain the broad beamwidth of an antenna, a TM010 mode and a ZOR mode are combined at the same
frequency. By using the omni-directional radiation pattern of a ZOR mode, the E-plane beamwidth of a TM010
mode can easily be broadened. To generate a TM010 mode and a ZOR mode simultaneously, the mushroom
structure is inserted inside an etched hole of the rectangular patch. The hybrid antenna has the advantages of a
simple structure, a single-layered substrate, and a planar configuration even though two radiators are employed.
Its resonant frequency is independent of its physical length, so ZOR antennas are very compact. It has a uniform
vertical electric field towards the ground plane, so that ZOR antenna has the magnetic loop current along open
ended side wall. Thus the proposed low profile antenna omni-directionally radiates and covers a larger area.
Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth
DOI: 10.9790/2834-10330109 www.iosrjournals.org 9 | Page
References
[1]. R. Garg, P. Bhartia, I. Bahl, and A. Ittipiboon, Microstrip Antenna Design Handbook. Boston, MA: Artech House, 2000.
[2]. C. A. Balanis, Antenna Theory: Analysis and Design, 3rd ed. New York: Wiley, 2005.
[3]. T. P. Wong and K. M. Luk, “A wideband L-probe patch antenna array with wide beamwidth,” IEEE Trans. Antennas Propag., vol.
51, no. 10, pp. 3012–3014, Oct. 2003.
[4]. C. W. Su, S. K. Huang, and C. H. Lee, “CP microstrip antenna with wide beamwidth for GPS band application,” Electron. Lett.,
vol. 43, no. 20, Sep. 2007.
[5]. X. L. Bao and M. J. Ammann, “Dual-frequency dual circularly-polarized patch antenna with wide beamwidth,” Electron. Lett., vol.
44, no. 21, pp. 1233–1234, Oct. 2008.
[6]. Z.-S. Duan, S.-B. Qu, Y. Wu, and J.-Q. Zhang, “Wide bandwidth and broad beamwidth microstrip patch antenna,” Electron. Lett.,
vol. 45, no. 5, pp. 249–250, Feb. 2009.
[7]. S.-W.Qu, J.-L. Li, andQ.Xue, “Bowtie dipole antenna with wide beam width for base station application,” IEEE Antennas Wireless
Propag. Lett., vol. 6, pp. 293–295, 2007.
[8]. Z. N. Chen,W. K. Toh, and X. M. Qing, “A microstrip patch antenna with broadened beamwidth,” Microw. Opt. Technol. Lett., vol.
50, no. 7, pp. 1885–1888, Jul. 2008.
[9]. A. Sanada, C. Caloz, and T. Itoh, “Planar distributed structures with negative refractive properties,” IEEE Trans. Microwave Theory
Tech., vol. 52, no. 4, pp. 1252–1263, Apr. 2004.
[10]. A. Lai, C. Caloz, and T. Itoh, “Composite right/left-handed transmission line metamaterials,” IEEE Microwave Mag., vol. 5, no. 3,
pp. 34–50, Sep. 2004.
[11]. A. Lai, K. M. K. H. Leong, and T. Itoh, “Infinite wavelength resonant antennas with monopolar radiation pattern based on periodic
structures,” IEEE Trans. Antennas Propag., pp. 868–876, Mar. 2007.
[12]. J. G. Lee and J. H. Lee, “Zeroth order resonance loop antenna,” IEEE Trans. Antennas Propag., vol. 55, no. 3, pp. 994–997, Mar.
2007.
[13]. J.H.Park, Y.H.Ryu, J. G. Lee, and J. H. Lee, “Epsilon negative zeroth order resonator antenna,” IEEE Trans. Antennas Propag., vol.
55, no. 12, pp. 3710–3712, Dec. 2007.
[14]. S. T. Ko and J. H. Lee, “Miniaturized ENG ZOR antenna with high permeability material,” in IEEE AP-S/URSI, Canada, Jul. 2010.
[15]. Seung-Tae Ko and Jeong-Hae Lee, Hybrid Zeroth-Order Resonance Patch Antenna With Broad -Plane Beamwidth, IEEE Trans on
Antennas and Propagation, Vol. 61, No. 1, pp 19-25, Jan 2013.

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A010330109

  • 1. IOSR Journal of Electronics and Communication Engineering (IOSR-JECE) e-ISSN: 2278-2834,p- ISSN: 2278-8735.Volume 10, Issue 3, Ver. III (May - Jun.2015), PP 01-09 www.iosrjournals.org DOI: 10.9790/2834-10330109 www.iosrjournals.org 1 | Page Hybrid Zeroth-Order Resonance Patch Antenna with Improved Half Power Beamwidth Pearl Antonette Mendez1 , Deepthi Das Krishna2 1,2 (Department of Electronics & Communication, Rajagiri school of Engineering & Technology, Ernakulam, Kerala, India) Abstract: Antenna miniaturization is a critical issue in today’s wireless and communication systems. Omnidirectional antennas are useful for applications in wireless communication however these antennas radiate towards the broadside and antennas should protrude from ground for large radiation area. Several techniques to reduce antenna size have been proposed in the recent years. One approach is Metamaterial (MTM) based zeroth-order resonator (ZOR), ZOR antennas with the same physical size present better performance if compared to other techniques. The conventional rectangular patch antenna cannot radiate omni- directionally, despite of structural stability. Resonant frequencies of the conventional rectangular patch antenna depend on width and length of patch, and height of substrate because of finite wavelength. ZOR antennas are designed by using the ZOR mode- one of many attractive properties of the metamaterial antennas. The antenna utilizes the zeroth-order resonance (ZOR) mode of the mushroom structure and the TM010 mode of the conventional rectangular patch. If the directional radiation pattern of a TM010 mode and the omni-directional radiation pattern of a ZOR mode are combined at the same frequency, it is expected that the total radiation pattern would have the broader beamwidth. Keywords: Beam width, Fringing, Metamaterials, Microstrip antenna, Rectangular Patch Antenna, Zeroth order resonance (ZOR) antenna. I. Introduction A patch antenna (also known as a rectangular microstrip antenna) is a type of radio antenna with a low profile, which can be mounted on a flat surface. It consists of a flat rectangular sheet or "patch" of metal, mounted over a larger sheet of metal called a ground plane. The radiation mechanism arises from discontinuities at each truncated edge of the microstrip transmission line.[2] The radiation at the edges causes the antenna to act slightly larger electrically than its physical dimensions, so in order for the antenna to be resonant, a length of microstrip transmission line slightly shorter than one-half a wavelength at the frequency is used. The rectangular patch antenna is approximately a one-half wavelength long section of rectangular microstrip transmission line. When air is the antenna substrate, the length of the rectangular microstrip antenna is approximately one-half of a free-space wavelength. As the antenna is loaded with a dielectric as its substrate, the length of the antenna decreases as the relative dielectric constant of the substrate increases. The microstrip patch antennas have been one of the most popular antennas in modern wireless communication systems as they have several desirable attributes, such as a low-profile planar configuration, a light weight, a simple design principle, a low fabrication cost, and so on [1], [2]. The conventional rectangular patch antenna has a directional radiation pattern at the TM010 mode. It has a relatively narrow scanning range and hence it is difficult for the antenna to maintain a stable performance in the changing environments or the moving systems. This disadvantage created a need for an antenna with an enhanced beamwidth. For obtaining a broad beamwidth, many antennas using the various techniques have been reported. For example, by using the phase array patch structures [3], the multilayered structures [4]–[6], or the parasitic radiators [7], [8], it is possible to design the patch antennas with a broad beamwidth. However, they have several limitations such as a larger size, a difficult design, and a multi-layered structure. II. Rectangular Patch Antenna A patch antenna is usually constructed on a dielectric substrate, using the same materials and lithography processes used to make printed circuit boards. The most commonly employed microstrip antenna is a Rectangular patch. Dimensions of the patch are finite along the length and width and hence the fields at the edges undergo fringing. Radiation in patch antenna is due to the fringing field between the periphery of the patch and the ground plane which is a function of dimension of patch and substrate height. It increases with the height of the substrate. But as the height increases, surface waves which are unwanted radiations also increase, so an optimum value for substrate height should be chosen. Fringing makes the microstrip line look wider electrically compared to its physical dimensions. Since some of the waves travel in the substrate and some in air, an effective dielectric constant is introduces to account for fringing and the wave propagation in the line.
  • 2. Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth DOI: 10.9790/2834-10330109 www.iosrjournals.org 2 | Page 2.1 Rectangular Patch Antenna With Etched Hole A rectangular patch antenna with an etched rectangular hole is shown in fig 1. The rectangular hole is etched in the center of a patch [15]. In addition, a circular patch and a gap (gp)as a feeding structure are employed. A coaxial probe (50 ohms ) is directly connected with the circular patch. Therefore, the excited power is coupled to the rectangular patch through the circular patch. A TM010 mode can be generated in this structure like a conventional rectangular patch antenna. The dimensions of the antenna are as follows: Width of the substrate Ws=45mm, Length of the substrate Ls =40mm, width of the etched hole We =11mm, Length of the etched hole=6mm, gp=0.2mm, height of the substrate hs=3.175mm, Width of the patch Wp=15mm, Length of the patch Lp=10mm, permittivity=2.2 and δd = 0.0009. Fig. 1. Geometry of the rectangular patch antenna with an etched rectangular hole. III. Mushroom Antenna Mushroom antennas are made up of metamaterials which are synthetic material with unusual refractive properties, used for wireless systems. Their Optical and electromagnetic properties can be engineered by changing the geometry of its unit cells. Each artificial unit responds to the radiation from the source. The collective result is the material’s response to the electromagnetic wave that is broader than normal. It can step up radiated power of an antenna, stores energy reradiates, behaves as if it was much more larger. It is an infinite wavelength antenna where infinite wavelength occurs because the propagation constant is zero. Hence its frequency does not depend on its physical length, but on the reactance provided by its unit cell. A circular patch is directly connected with the coaxial probe, and a gap is inserted between the mushroom patch and circular patch. Therefore, an excited power is coupled from the circular patch to the mushroom patch. In general, the mushroom antenna has an infinite wavelength mode at specific non-zero frequency called a ZOR mode. The resonance frequency of a ZOR mode is determined by the area of a patch, the radius of a via, and the height of a mushroom antenna. The dimensions of the antenna are as follows: Width of the substrate Ws=45mm, Length of the substrate Ls =40mm, width of the etched hole We=11mm, Length of the etched hole=6mm, gp=0.2mm, height of the substrate hs=3.175mm, Width of the patch Wp=15mm, Length of the patch Lp=10mm,ε=2.2 and δd = 0.0009. IV. Hybrid ZOR Antenna Fig 2: Hybrid ZOR antenna
  • 3. Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth DOI: 10.9790/2834-10330109 www.iosrjournals.org 3 | Page To combine two modes at the same frequency, the structure where the mushroom ZOR antenna is inserted in the etched pattern of a rectangular patch antenna, is designed. The antenna utilizes the zeroth-order resonance (ZOR) mode [9], [10] of the mushroom structure and the TM010 mode of the conventional rectangular patch .Therefore, the proposed antenna is composed of two radiators. This antenna will be called as a hybrid ZOR antenna since it operates with the TM010 mode and the ZOR mode at the same frequency with a single feed. First, the rectangular etched hole allows the patch antenna to have a lower resonance frequency of the TM010 mode without changing the radiation pattern, the E-plane HPBW, and the size of an antenna. Second, the mushroom ZOR antenna has the omni-directional pattern. If it is assumed that the resonance frequency of the ZOR mode is the same as that of the TM010 mode and two modes are generated simultaneously, the directional radiation pattern and the omni-directional pattern can be combined. It is expected that the total radiation pattern would have the broader beamwidth. First, the etched rectangular hole is patterned on the center of the rectangular patch and, then, the mushroom ZOR antenna is inserted inside the hole. At the ZOR mode, an equivalent horizontal magnetic loop current is generated inside the mushroom structure, resulting in a low- profile omni-directional radiation pattern [11]–[14]. This proposed antenna has structurally several advantages. First, the antenna needs only single-layered substrate and maintains a planar configuration. Second, although the antenna has two radiators, a small size can be achieved because the mushroom ZOR antenna is added inside the etched hole. Finally, it has a simple structure. In order to excite the TM010 mode of an outer patch and the ZOR mode of an inner mushroom patch simultaneously, a circular feeding patch is inserted between two patches. The circular patch is directly connected to the coaxial probe. Thus, two radiators receive the incident power from the single feed. In addition, two gaps of gp and gm are added between the circular patch and two radiators in order to independently control the injected power to each antenna. V. Figures And Tables Fig 3: Rectangular patch antenna with etched hole width= 3mm Fig 4: Resonant frequency of Rectangular patch antenna with etched hole width= 3mm
  • 4. Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth DOI: 10.9790/2834-10330109 www.iosrjournals.org 4 | Page Fig 5: Rectangular patch antenna with etched hole width=11mm Fig 6: Resonant frequency of Rectangular patch antenna with etched hole width= 3mm Fig 7: Radiation efficiency of Rectangular patch antenna
  • 5. Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth DOI: 10.9790/2834-10330109 www.iosrjournals.org 5 | Page Fig 8: Resonant frequency of Rectangular patch antenna with etched hole width= 5mm Fig 9: Resonant frequency of Rectangular patch antenna with etched hole width= 7mm Fig 10: Resonant frequency of Rectangular patch antenna with etched hole width= 9mm
  • 6. Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth DOI: 10.9790/2834-10330109 www.iosrjournals.org 6 | Page Fig 11: Mushroom antenna Fig 12: Resonant frequency of Mushroom antenna Fig 13: HPBW of Mushroom Antenna
  • 7. Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth DOI: 10.9790/2834-10330109 www.iosrjournals.org 7 | Page Fig 14: Hybrid ZOR antenna Fig 15: Resonant frequency of hybrid ZOR antenna Fig 16: Radiation efficiency of hybrid antenna
  • 8. Hybrid Zeroth-Order Resonance Patch Antenna with improved half power beamwidth DOI: 10.9790/2834-10330109 www.iosrjournals.org 8 | Page Fig 17: HPBW of hybrid ZOR antenna Table 1: Effect of Resonant frequency on etched hole width for rectangular patch antenna with etched hole Sl no Etched hole width (mm) Resonant frequency (GHz) 1 3 5.2 2 5 5.05 3 7 4.8 4 9 4.49 5 11 4.13 Table 2: Comparison of the parameters of the proposed antenna with Rectangular Patch Parameters Rectangular Patch Mushroom antenna Hybrid ZOR antenna Resonant frequency 4.22 GHz 13.9 GHz 4.31 GHz Half power beam width 24.8° 117.5° 99.7° Radiation efficiency 75% 20.14% 69% Radiated power 0.23 W 0.0053 W 0.056 W VI. Summary Of Results Rectangular patch antenna has very low HPBW and hence is not ideal in moving environments because of its very low scanning range. By employing the rectangular etched hole, the resonance frequency of the patch antenna is down-shifted without changing the HPBW and the size of the antenna. The E-plane HPBW is broadened compared with that of the conventional patch antenna. The proposed antenna has not only the broader E-plane HPBW but also the smaller size than the conventional rectangular patch antenna. Even though mushroom antenna has the maximum HPBW, it has very low radiation efficiency and cannot be used. So when both antennas are combined, the E Plane beamwidth as well as radiation efficiency is increased. VII. Conclusion A hybrid ZOR patch antenna having the broad E-plane beamwidth is designed and simulated. In order to obtain the broad beamwidth of an antenna, a TM010 mode and a ZOR mode are combined at the same frequency. By using the omni-directional radiation pattern of a ZOR mode, the E-plane beamwidth of a TM010 mode can easily be broadened. To generate a TM010 mode and a ZOR mode simultaneously, the mushroom structure is inserted inside an etched hole of the rectangular patch. The hybrid antenna has the advantages of a simple structure, a single-layered substrate, and a planar configuration even though two radiators are employed. Its resonant frequency is independent of its physical length, so ZOR antennas are very compact. It has a uniform vertical electric field towards the ground plane, so that ZOR antenna has the magnetic loop current along open ended side wall. Thus the proposed low profile antenna omni-directionally radiates and covers a larger area.
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