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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3691
Dual Band Low Profile MPA with I-Shaped MTM Unit Cell for Satellite
Communication
Priya Kardam1, Dharmendra Kumar2
1M.Tech. Scholar, KIET Group of Institutions, Ghaziabad, Uttar Pradesh, India
2Associate Professor, KIET Group of Institutions, Ghaziabad, Uttar Pradesh, India.
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract - A rectangular MPA having an etched I-shape
metamaterial structure with in the ground plane is suggested
in this work. The low profile design, having electrical size
0.43λo × 0.54λo × 0.06λo (i.e., 11mm×14mm×1.6mm), is
designed to operate at 12.2GHz. The metamaterial unit cell
included in the ground plane introduces another resonant
peak (at 10.5GHz) to make the antenna dual band. The
simulation process is conducted with the help of hfss v.15
simulation software. The outcomes of the simulation show an
improvement in the antenna fractional bandwidth and gain.
The antenna results in a fractional bandwidth of 6.58% with
the central resonant frequency of 10.5GHz and 2.41% with
12.2GHz. The simulated value of peak gain is 4.81dB at
10.5GHz and 1.33dB at 12.2GHz. The proposed antenna also
shows good impedance matching condition and results in a
return loss of -19.43dB at 10.5GHz and -17.56dB at 12.2GHz.
The design also shows an increase in antenna efficiency. The
resulted efficiency of the antenna is 80%. I-shaped
metamaterial structurecreatedwithinitsbottomsurfaceadds
a 46.63% miniaturization in the radiator (patch) area of the
proposed antenna. The MTM-antenna designed in the work is
suitable for the applications in X-band (e.g. radar
communication) and Ku-band (e.g. satellite communication).
The antenna also has a notch band between the two bands i.e.
10.8GHz to 12.1 GHz which avoid interference between two
resonant regions.
Keywords- MTM (metamaterial), MPA (Microstrip Patch
Antenna), miniaturization, hfss (high frequency structure
simulator).
1. INTRODUCTION
Numerous benefits of patch antennas like compact
dimensions, low profile, effective in cost and easyintermsof
fabrication make them famous among the researchers[1-2].
These advantages make them most suited antennas for the
wireless communication applications.
An artificially created periodic media that finds its
characteristic features (in terms of electromagnetic
responses) totally different from its base material is famous
by the name Metamaterial [3]. The periodic structure, either
created by slots in base material or by arranging the similar
materials in periodic manner, results in double negative
(DNG) metamaterial which has both its permittivity and
permeability in the negative region.Suchcharacteristicwere
first detected and studied by Veselago [4]. A paper by Smith
et al had experimentally verified the characterization given
by Veselago about DNG material [5]. After this, these
metamaterial structures are identified and applied in the
antenna application for improving the antenna radiation
characteristics. These metamaterialsinsertedintheantenna
structures have not onlyshowedanimprovementinantenna
parameters like gain, return loss and directivity but also
resulted in miniaturization in the antenna dimensions [6-
11].
The work in this paper aims to simulate a
rectangular microstrip patch antenna having an I-shape
metamaterial unit cell created by etching within the ground
surface. The structure is modeledto resonateat10.5GHzand
12.2GHz. The simulation work of the design is conducted
using hfss v15 simulation software and the outcomes of the
simulation are illustrated in the paper. The proposed
antenna shows 46.63% miniaturization with respect to the
area of patch in contrast to that of the regular patch area at
same resonant frequency. The proposed antenna shows an
enhancement with respect to both Gain and fractional
bandwidth.
2. DESIGN ASPECTS OF PROPOSED MTM-ANTENNA
The geometrical aspects related to the proposed
MTM antenna is depicted in the figure 1 below. The figure
demonstrates upper and lower surface of the simulated
structure. The lower surface of the designed patch antenna,
called as ground plane, is etched with an I-shape
metamaterial unit cell placed symmetrically at the center of
the ground. The rectangular patch with inset feed using a
microstrip line is placed on a FR4 epoxy glass material
having 1.6mm of height, relative dielectric permittivity εr
=4.4 and the loss-factor tanδ=0.02. Other geometrical
parameters for the simulated structure are illustrated in the
table given below.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3692
(a)
(b)
(c)
Figure 1. (a) Upper surface having patch, (b) Ground
plane with metamaterial unit cell and (c) overall hfss
model of the designed antenna
TABLE I
Proposed Antenna: Dimensions
Facet Units (mm) Facet Units (mm)
Lg 11 s 1
Wg 14 Ls 3
Lp 5 Ws 2.5
Wp 6 u 1.75
Lm 3.5 v 1.25
t 2 w 1
x 0.25
The microstripfeedlineisconnectedandpositioned
to result the best possible impedancematchingcondition for
the antenna. The inset feeding is doneto reducethespurious
radiation near the feed patch interface.
3. METAMATERIAL UNIT CELL EQUIVALENT
CIRCUIT
An unit cell of the metamaterial structure included
in the ground plane denotes LC resonant circuit in its
equivalent model resonating at particular resonant
frequency. The metal strips in the unit cell acts like an
inductor whereas the gaps in between acts like capacitors.
These unit cells when exposed with the electromagnetic
radiation either stores or reflect all the waves passing
through them.
The equivalent model of a metamaterial cell is
depicted in the fig.2.
Figure 2. MTM-unit cell equivalent circuit
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3693
MTM unit cell’s resonant frequency is given as,
Here, Leq and Ceq denote the equivalent values of
inductance and capacitance for the metamaterial unit cell
respectively.
4. SIMULATED ANTENNA PARAMETERS
Return loss (S11 dB) - The parameter of reflection (S11) for
the simulated resonator is drawn in the fig.3. The designed
antenna receives good impedance matching. The simulated
value of the parameter S11 is -19.43dB at the resonating
frequency of 10.5GHz and -17.56dB at 12.2GHz. Around
these center frequencies, the resulted fractional BW for the
designed antenna is6.58%and2.41%respectively.Thus,the
antenna shows an improvement in terms of bandwidth.
Figure 3. Graph of simulated return loss
Gain and Directivity- An integrated plot of gain and
directivity of the suggested antenna is shown in the fig. 4
below. The peak gain resulted at the resonant frequency of
10.5GHz is 4.8dB and 12.2GHz is 1.33dB. The measures of
peak directivity are 5.89dB and 4.47dB respectively.
Figure 4. Integrated plot of gain and directivity vs
frequency
Antenna Efficiency- The capability of an antenna to
generate radiated power from the radio-frequency power is
termed as its efficiency. The proposed antenna is 80%
efficient.
Radiation Pattern- A semi-omnidirectional radiation
pattern depicted in the fig.5(a) is shown by the proposed
antenna. The radiation pattern shown is well suited for the
satellite and radar communication applications.
(a)
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3694
(b)
Figure 5 (a) Pattern of Radiation with varying
theta,(b) Polar plot with respect to total gain.
Current distributions- The distributions ofcurrentdensity
for the resonating patch surface and the ground suface
having metamaterial unit-cell are drawn in the fig.6.
Figure 6. Current distribution across the metamaterial
unit cell
Co-Polarization and Cross-Polarization- The E and H
plane’s Co. and X-polarizations plots are drawn in the fig.7.
The measures of both the polarizations for both the planes
are also given in the table 2 below.
(a)
(b)
Figure 7. (a) E-Plane’s Co. & X-polarization, (b) H-
Plane’s Co. & X-polarization
TABLE II
Measures of Co. & X-Polarization
Plane Peak Co-pol.(dB)
Peak Cross-
pol.(dB)
E-Plane 4.35 -33.78
H-plane -0.40 -34.78
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3695
Voltage Standing Wave Ratio (VSWR) - The simulated
graph for VSWR vs frequency is depicted in the fig.8. The
measure of VSWR for the suggested antenna is 1.86dB with
the resonant frequency of 10.5GHz and 2.23dB at 12.2GHz.
Figure 8. Graph of VSWR vs frequency
Miniaturization- The required patch area for a regular
microstrip patch antenna modeled with a 12.2GHz
resonating frequency is 38.12 mm². The effective patch area
for the designed antenna is 26 mm². Hence, the proposed
antennas results in 46.63% miniaturization in the patch
dimensions.
5. CONCLUSION
Metamaterial-inspired rectangularMPAisdescribed
and simulated in the paper. All important antenna
parameters are calculated and the results obtained are
illustrated in the paper. The antenna, designed with the
resonant frequencies of 10.5GHz and 12.2GHz, has not only
shown an improvement in antenna gain and fractional
bandwidth but also added 46.63% miniaturization in
antenna’s patch area.Thedesignalsoshowsgoodimpedance
matching condition as the parameterofreflection(S11)atthe
resonating frequency is quite low.
The desined antenna finds its application in the X-
band and Ku-band of electromagnetic spectrum. The bands
are useful for satellite communication and radar
applications. The antenna has semi-omnidirectional
radiation pattern, so it is well suited for applications in
satellite communication.
Table 3 makes a comparison between the previous
literatures and antenna proposed in the paper. The antenna
shows improvement in terms of gain and fractional
bandwidth.
TABLE III
Comparison among Previously Designed Antennas and
Proposed Antenna
References
Resonating
Frequencies
(GHz)
Fractional
Bandwidth
(%)
Peak Gain
(dB)
[12]
1.35
3.75
4.4
2.6
0.4
2.6
[13]
2.49
3.66
3.2
2.74
-0.5
1.27
[14]
3.51
5.76
3.4
2.43
1.3
5
[15]
3.65
5.77
4.33
2.06
3.1
5.8
Suggested
Antenna
10.5
12.2
6.58
2.41
4.81
1.33
To get more improvement in the antenna
parameters and to get high degree of miniaturization, more
number of unit cells can be constructed in place of one. By
using the array of unit cells, it is also possible to receive
double-band or multi band response.
REFERENCES
[1] C.A.Balanis, Antenna Theory: Analysis and Design, John
Wiley & Sons, Hoboken, NJ, USA, 2005
[2] K.-L. Wong, Compact and Broadband Microstrip
Antennas, Wiley, New York, NY, USA, 2002
[3] M.Lapineand S. Tretyakov,”Contemporary notes on
metamaterials”, IET Microwaves,AntennasandPropagation,
vol. 1, no,1, pp.3-11,2007
[4] V.G.Veselago,“The electrodynamics of substances with
simultaneous negative values of 𝜀 and 𝜇,” Soviet Physics
Uspekhi, vol. 10,no.4,pp.509–514,1968
[5] D. R. Smith, W. J. Padilla, D. C. Vier, S. C. Nemat-Nasser,
and S. Schultz, “Composite medium with simultaneous
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3696
negative permeability and permittivity,” Physical Review
Letters, vol.84, no.18, pp.4184–4187,2000.
[6] C.-C.Chenand J.L.Volakis,“Bandwidthbroadeningofpatch
antennas using non uniform substrates,”Microwave and
Optical Technology Letters, vol.47, no.5, pp.421–423,2005
[7] J. Zhu and G. V. Eleftheriades, “A compact transmission
line metamaterial antenna with extended bandwidth,” IEEE
Antennas and Wireless Propagation Letters, vol.8, pp.295–
298, 2009
[8] B.-I.Wu, W.Wang, J.PachecoJr., X.Chen, T.M.Grzegorczyk,
and J.A.Kong,“A study of using metamaterials as antenna
substrate to enhance gain,” Progress in Electromagnetics
Research, vol.51,pp.295–328,2005
[9] B.-I.Wu, W.Wang, J.Pachecoetal.,“An isotropic
metamaterials as antenna substrate to enhance directivity,”
Microwave and Optical Technology Letters, vol.48, no.4, p
p.680–683,2006
[10] Z.-B. Weng, Y.-C. Jiao, G. Zhao, and F.-S. Zhang, “Design
and experiment of one dimension and two dimension
metamaterial structures for directive emission,” Progressin
Electromagnetics Research, vol.70,pp.199–209,2007
[11] H. Xu, Z. Zhao, Y. Lv, C. Du, and X. Luo, “Metamaterial
superstrate and electromagnetic band-gapsubstrateforhigh
directive antenna,” International Journal of Infrared and
MillimeterWaves,vol.29,no.5,pp.493–498,2008
[12] V. Rajesh kumar, S. Raghvan “A compact CSRR loaded
dual band microstrip patch antenna for wireless
applications,” IEEE Int. Conference on Computational
Intelligence and Computing Research, 978-1-4799-1579-
2,2013
[13] Lee, Tse, Hao, and Clive G. Parini “A compact microstrip
antenna with improved bandwidth using CSRR loading,”
IEEE,2007, 1-1244-0878-4/07
[14] Bhavna Thakur, Ashwini Kunte “Compact dual-band
patch antenna using triangular complementary split ring
resonators for WiMax/WLAN,” International Conference on
Communication, Information & Computing Technology
(ICCICT), Feb. 2-3, Mumbai, 2018
[15] Bhavna Thakur, Ashwini Kunte “Compact dual band
patch antenna using meandered complementary split ring
resonators,” 3rd International Conference for Convergence
in Technology (I2CT), Pune,Apr 06-08-2018

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IRJET - Dual Band Low Profile MPA with I-shaped MTM Unit Cell for Satellite Communication

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3691 Dual Band Low Profile MPA with I-Shaped MTM Unit Cell for Satellite Communication Priya Kardam1, Dharmendra Kumar2 1M.Tech. Scholar, KIET Group of Institutions, Ghaziabad, Uttar Pradesh, India 2Associate Professor, KIET Group of Institutions, Ghaziabad, Uttar Pradesh, India. ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - A rectangular MPA having an etched I-shape metamaterial structure with in the ground plane is suggested in this work. The low profile design, having electrical size 0.43λo × 0.54λo × 0.06λo (i.e., 11mm×14mm×1.6mm), is designed to operate at 12.2GHz. The metamaterial unit cell included in the ground plane introduces another resonant peak (at 10.5GHz) to make the antenna dual band. The simulation process is conducted with the help of hfss v.15 simulation software. The outcomes of the simulation show an improvement in the antenna fractional bandwidth and gain. The antenna results in a fractional bandwidth of 6.58% with the central resonant frequency of 10.5GHz and 2.41% with 12.2GHz. The simulated value of peak gain is 4.81dB at 10.5GHz and 1.33dB at 12.2GHz. The proposed antenna also shows good impedance matching condition and results in a return loss of -19.43dB at 10.5GHz and -17.56dB at 12.2GHz. The design also shows an increase in antenna efficiency. The resulted efficiency of the antenna is 80%. I-shaped metamaterial structurecreatedwithinitsbottomsurfaceadds a 46.63% miniaturization in the radiator (patch) area of the proposed antenna. The MTM-antenna designed in the work is suitable for the applications in X-band (e.g. radar communication) and Ku-band (e.g. satellite communication). The antenna also has a notch band between the two bands i.e. 10.8GHz to 12.1 GHz which avoid interference between two resonant regions. Keywords- MTM (metamaterial), MPA (Microstrip Patch Antenna), miniaturization, hfss (high frequency structure simulator). 1. INTRODUCTION Numerous benefits of patch antennas like compact dimensions, low profile, effective in cost and easyintermsof fabrication make them famous among the researchers[1-2]. These advantages make them most suited antennas for the wireless communication applications. An artificially created periodic media that finds its characteristic features (in terms of electromagnetic responses) totally different from its base material is famous by the name Metamaterial [3]. The periodic structure, either created by slots in base material or by arranging the similar materials in periodic manner, results in double negative (DNG) metamaterial which has both its permittivity and permeability in the negative region.Suchcharacteristicwere first detected and studied by Veselago [4]. A paper by Smith et al had experimentally verified the characterization given by Veselago about DNG material [5]. After this, these metamaterial structures are identified and applied in the antenna application for improving the antenna radiation characteristics. These metamaterialsinsertedintheantenna structures have not onlyshowedanimprovementinantenna parameters like gain, return loss and directivity but also resulted in miniaturization in the antenna dimensions [6- 11]. The work in this paper aims to simulate a rectangular microstrip patch antenna having an I-shape metamaterial unit cell created by etching within the ground surface. The structure is modeledto resonateat10.5GHzand 12.2GHz. The simulation work of the design is conducted using hfss v15 simulation software and the outcomes of the simulation are illustrated in the paper. The proposed antenna shows 46.63% miniaturization with respect to the area of patch in contrast to that of the regular patch area at same resonant frequency. The proposed antenna shows an enhancement with respect to both Gain and fractional bandwidth. 2. DESIGN ASPECTS OF PROPOSED MTM-ANTENNA The geometrical aspects related to the proposed MTM antenna is depicted in the figure 1 below. The figure demonstrates upper and lower surface of the simulated structure. The lower surface of the designed patch antenna, called as ground plane, is etched with an I-shape metamaterial unit cell placed symmetrically at the center of the ground. The rectangular patch with inset feed using a microstrip line is placed on a FR4 epoxy glass material having 1.6mm of height, relative dielectric permittivity εr =4.4 and the loss-factor tanδ=0.02. Other geometrical parameters for the simulated structure are illustrated in the table given below.
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3692 (a) (b) (c) Figure 1. (a) Upper surface having patch, (b) Ground plane with metamaterial unit cell and (c) overall hfss model of the designed antenna TABLE I Proposed Antenna: Dimensions Facet Units (mm) Facet Units (mm) Lg 11 s 1 Wg 14 Ls 3 Lp 5 Ws 2.5 Wp 6 u 1.75 Lm 3.5 v 1.25 t 2 w 1 x 0.25 The microstripfeedlineisconnectedandpositioned to result the best possible impedancematchingcondition for the antenna. The inset feeding is doneto reducethespurious radiation near the feed patch interface. 3. METAMATERIAL UNIT CELL EQUIVALENT CIRCUIT An unit cell of the metamaterial structure included in the ground plane denotes LC resonant circuit in its equivalent model resonating at particular resonant frequency. The metal strips in the unit cell acts like an inductor whereas the gaps in between acts like capacitors. These unit cells when exposed with the electromagnetic radiation either stores or reflect all the waves passing through them. The equivalent model of a metamaterial cell is depicted in the fig.2. Figure 2. MTM-unit cell equivalent circuit
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3693 MTM unit cell’s resonant frequency is given as, Here, Leq and Ceq denote the equivalent values of inductance and capacitance for the metamaterial unit cell respectively. 4. SIMULATED ANTENNA PARAMETERS Return loss (S11 dB) - The parameter of reflection (S11) for the simulated resonator is drawn in the fig.3. The designed antenna receives good impedance matching. The simulated value of the parameter S11 is -19.43dB at the resonating frequency of 10.5GHz and -17.56dB at 12.2GHz. Around these center frequencies, the resulted fractional BW for the designed antenna is6.58%and2.41%respectively.Thus,the antenna shows an improvement in terms of bandwidth. Figure 3. Graph of simulated return loss Gain and Directivity- An integrated plot of gain and directivity of the suggested antenna is shown in the fig. 4 below. The peak gain resulted at the resonant frequency of 10.5GHz is 4.8dB and 12.2GHz is 1.33dB. The measures of peak directivity are 5.89dB and 4.47dB respectively. Figure 4. Integrated plot of gain and directivity vs frequency Antenna Efficiency- The capability of an antenna to generate radiated power from the radio-frequency power is termed as its efficiency. The proposed antenna is 80% efficient. Radiation Pattern- A semi-omnidirectional radiation pattern depicted in the fig.5(a) is shown by the proposed antenna. The radiation pattern shown is well suited for the satellite and radar communication applications. (a)
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3694 (b) Figure 5 (a) Pattern of Radiation with varying theta,(b) Polar plot with respect to total gain. Current distributions- The distributions ofcurrentdensity for the resonating patch surface and the ground suface having metamaterial unit-cell are drawn in the fig.6. Figure 6. Current distribution across the metamaterial unit cell Co-Polarization and Cross-Polarization- The E and H plane’s Co. and X-polarizations plots are drawn in the fig.7. The measures of both the polarizations for both the planes are also given in the table 2 below. (a) (b) Figure 7. (a) E-Plane’s Co. & X-polarization, (b) H- Plane’s Co. & X-polarization TABLE II Measures of Co. & X-Polarization Plane Peak Co-pol.(dB) Peak Cross- pol.(dB) E-Plane 4.35 -33.78 H-plane -0.40 -34.78
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3695 Voltage Standing Wave Ratio (VSWR) - The simulated graph for VSWR vs frequency is depicted in the fig.8. The measure of VSWR for the suggested antenna is 1.86dB with the resonant frequency of 10.5GHz and 2.23dB at 12.2GHz. Figure 8. Graph of VSWR vs frequency Miniaturization- The required patch area for a regular microstrip patch antenna modeled with a 12.2GHz resonating frequency is 38.12 mm². The effective patch area for the designed antenna is 26 mm². Hence, the proposed antennas results in 46.63% miniaturization in the patch dimensions. 5. CONCLUSION Metamaterial-inspired rectangularMPAisdescribed and simulated in the paper. All important antenna parameters are calculated and the results obtained are illustrated in the paper. The antenna, designed with the resonant frequencies of 10.5GHz and 12.2GHz, has not only shown an improvement in antenna gain and fractional bandwidth but also added 46.63% miniaturization in antenna’s patch area.Thedesignalsoshowsgoodimpedance matching condition as the parameterofreflection(S11)atthe resonating frequency is quite low. The desined antenna finds its application in the X- band and Ku-band of electromagnetic spectrum. The bands are useful for satellite communication and radar applications. The antenna has semi-omnidirectional radiation pattern, so it is well suited for applications in satellite communication. Table 3 makes a comparison between the previous literatures and antenna proposed in the paper. The antenna shows improvement in terms of gain and fractional bandwidth. TABLE III Comparison among Previously Designed Antennas and Proposed Antenna References Resonating Frequencies (GHz) Fractional Bandwidth (%) Peak Gain (dB) [12] 1.35 3.75 4.4 2.6 0.4 2.6 [13] 2.49 3.66 3.2 2.74 -0.5 1.27 [14] 3.51 5.76 3.4 2.43 1.3 5 [15] 3.65 5.77 4.33 2.06 3.1 5.8 Suggested Antenna 10.5 12.2 6.58 2.41 4.81 1.33 To get more improvement in the antenna parameters and to get high degree of miniaturization, more number of unit cells can be constructed in place of one. By using the array of unit cells, it is also possible to receive double-band or multi band response. REFERENCES [1] C.A.Balanis, Antenna Theory: Analysis and Design, John Wiley & Sons, Hoboken, NJ, USA, 2005 [2] K.-L. Wong, Compact and Broadband Microstrip Antennas, Wiley, New York, NY, USA, 2002 [3] M.Lapineand S. Tretyakov,”Contemporary notes on metamaterials”, IET Microwaves,AntennasandPropagation, vol. 1, no,1, pp.3-11,2007 [4] V.G.Veselago,“The electrodynamics of substances with simultaneous negative values of 𝜀 and 𝜇,” Soviet Physics Uspekhi, vol. 10,no.4,pp.509–514,1968 [5] D. R. Smith, W. J. Padilla, D. C. Vier, S. C. Nemat-Nasser, and S. Schultz, “Composite medium with simultaneous
  • 6. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 07 | July 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 3696 negative permeability and permittivity,” Physical Review Letters, vol.84, no.18, pp.4184–4187,2000. [6] C.-C.Chenand J.L.Volakis,“Bandwidthbroadeningofpatch antennas using non uniform substrates,”Microwave and Optical Technology Letters, vol.47, no.5, pp.421–423,2005 [7] J. Zhu and G. V. Eleftheriades, “A compact transmission line metamaterial antenna with extended bandwidth,” IEEE Antennas and Wireless Propagation Letters, vol.8, pp.295– 298, 2009 [8] B.-I.Wu, W.Wang, J.PachecoJr., X.Chen, T.M.Grzegorczyk, and J.A.Kong,“A study of using metamaterials as antenna substrate to enhance gain,” Progress in Electromagnetics Research, vol.51,pp.295–328,2005 [9] B.-I.Wu, W.Wang, J.Pachecoetal.,“An isotropic metamaterials as antenna substrate to enhance directivity,” Microwave and Optical Technology Letters, vol.48, no.4, p p.680–683,2006 [10] Z.-B. Weng, Y.-C. Jiao, G. Zhao, and F.-S. Zhang, “Design and experiment of one dimension and two dimension metamaterial structures for directive emission,” Progressin Electromagnetics Research, vol.70,pp.199–209,2007 [11] H. Xu, Z. Zhao, Y. Lv, C. Du, and X. Luo, “Metamaterial superstrate and electromagnetic band-gapsubstrateforhigh directive antenna,” International Journal of Infrared and MillimeterWaves,vol.29,no.5,pp.493–498,2008 [12] V. Rajesh kumar, S. Raghvan “A compact CSRR loaded dual band microstrip patch antenna for wireless applications,” IEEE Int. Conference on Computational Intelligence and Computing Research, 978-1-4799-1579- 2,2013 [13] Lee, Tse, Hao, and Clive G. Parini “A compact microstrip antenna with improved bandwidth using CSRR loading,” IEEE,2007, 1-1244-0878-4/07 [14] Bhavna Thakur, Ashwini Kunte “Compact dual-band patch antenna using triangular complementary split ring resonators for WiMax/WLAN,” International Conference on Communication, Information & Computing Technology (ICCICT), Feb. 2-3, Mumbai, 2018 [15] Bhavna Thakur, Ashwini Kunte “Compact dual band patch antenna using meandered complementary split ring resonators,” 3rd International Conference for Convergence in Technology (I2CT), Pune,Apr 06-08-2018