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Performance Enhancement of Rectangular Microstrip
Patch Antenna Using Double H Shaped Metamaterial
Preet Kaur1*, S. K. Aggarwal1**, and Asok De2***
1YMCA University of Science and Technology, Faridabad, India
2National Institute of Technology, Patna, India
*e-mail: preetmoar@gmail.com
**e-mail: sa_3264@yahoo.co.in
***e-mail: asok.de@gmail.com
Received in final form June 6, 2016
Abstract—In this paper a high performance rectangular microstrip patch antenna (RMPA) has been
designed using double H shaped metamaterial. First, the double H shaped metamaterial has been designed
and optimized at 5.2 GHz resonant frequency of patch antenna. It has been found that embedding of this
metamaterial into the substrate beneath the reference patch antenna improves its return loss and
bandwidth without changing the resonant frequency and gain. To further enhance the gain and efficiency
of the metamaterial embedded RMPA a superstrate of double H shaped metamaterial has been applied at
the distance of l/3 over it. Finally, a high gain, broadband and good impedance matched metamaterial
inspired RMPA has been obtained. The proposed antenna was simulated and optimized using HFSS
software. The prototype antenna has been fabricated and measured results of the proposed antenna are
found to be in good agreement with the simulated results.
DOI: 10.3103/S0735272716110030
1. INTRODUCTION
In modern wireless and electronics systems the demand for compact, high gain, broad-band, low-cost and
light weight radiator with single feeding system has been increased substantially [1, 2]. Conventional
rectangular microstrip patch antenna (RMPA) compatible for wireless application has low profile, simple
structure, low cost, ease of fabrication and has simple feeding system, but this antenna has low gain and
narrow bandwidth because of the influence of surface wave on its radiation pattern [3]. In order to solve this
problem a microstrip patch array antenna can be used, but the complex feeding system and lower radiation
efficiency limit its application.
Recently, the researchers have proposed the utilization of metamaterial to design antennas with enhanced
performance and reduced profile [1]. Metamaterials are artificial materials formed by embedding specific
inclusion in host media and can be engineered to have desired electromagnetic properties.
Some of these materials have negative permittivity or permeability. If both permittivity and permeability
are negative at the same frequency, then these materials are called left handed materials and exhibit negative
index of refraction [4]. Several works have been dedicated to the improvement of the performance of
antennas using metamaterials [5–13].
Double H shaped metamaterial is a double negative (DNG) resonant material [14]. In [15] we have
presented a design of compact antenna using this resonant material, but the antenna has low gain. In this
paper double H shaped resonator is embedded underneath the patch antenna to improve the impedance
matching and to increase bandwidth without reducing the gain. To further improve the gain of the developed
antenna a superstrate of double H shaped metamaterial has been added into the structure at the distance of
l/3. The gain of 6.58 dB has been achieved, which is good result for a patch antenna.
496
ISSN 0735-2727, Radioelectronics and Communications Systems, 2016, Vol. 59, No. 11, pp. 496–501. © Allerton Press, Inc., 2016.
Original Russian Text © P. Kaur, S.K. Aggarwal, A. De, 2016, published in Izvestiya Vysshikh Uchebnykh Zavedenii, Radioelektronika, 2016, Vol. 59, No. 11,
pp. 29–36.
2. DESIGN AND RESULTS OF REFERENCE RMPA
2.1. Design and Results of Reference Antenna
Reference antenna has been designed based on FR4 epoxy substrate with dielectric constant 4.4 and loss
tangent 0.0025 at resonant frequency of 5.2 GHz using transmission line equations [16]. The designed
reference rectangular patch antenna has been simulated and optimized using HFSS software.
The length and width of the optimized patch antenna are 17.6´13.2 mm, respectively. The ground size
dimensions are 41.59´35.9 mm and the antenna is fed by inset microstrip line. The prototype of the
optimized reference antenna was fabricated (Fig. 1). We measured its reflection response using vector
network analyzer. Figure 2 demonstrates the simulated and measured reflection coefficient S11 of the
reference RMPA. As one can observe (Fig. 2), the antenna resonates at 5.2 GHz with –11.68 dB reflection
coefficient and it provides 70 MHz bandwidth. The gain of the reference antenna is 4.58 dB (Fig. 3). Figure 4
shows the radiation patterns of the antenna in Eand Hplanes.
3. DESIGN AND RESULTS OF DOUBLE H SHAPED RESONATOR
To improve the performance parameters of RMPA without altering its resonant frequency, a double H
shaped metamaterial has been designed. Its permittivity and permeability are negative at resonant frequency
(5.2 GHz) of the reference antenna. A unit cell of double H shaped resonator has been developed and
simulated using HFSS software (Fig. 5). The optimized geometrical parameters of the resonator are as
follows: length L1= 5.8 mm, L2= 5.8 mm, L3= 4.8 mm and width W1= 0.5 mm.
RADIOELECTRONICS AND COMMUNICATIONS SYSTEMS Vol. 59 No. 11 2016
PERFORMANCE ENHANCEMENT OF RMPA USING DOUBLE H SHAPED METAMATERIAL 497
Fig. 1. Fig. 2.
Fig. 4.Fig. 3.
246 810f, GHz
S11,dB
–2
–4
–6
–8
–10
–12
Simulated
Measured
24 6 8 10f, GHz
0
–5
–10
–15
–20
–25
Gain, dB
–60°
–90°
–120°
–150°
–180°
–30°
0°
30°
60°
90°
120°
150°
–8
–16
–24
–30
E-plane
H-plane
The effective permeability µrand permittivity er(Fig. 6) of double H shaped resonator are calculated
based on Sparameters using the Nicolson–Ross–Weir (NRW) approach by the following equations [17–19]:
mw
r
cv
dv
=-
×+
21
1
2
2
()
()i, (1)
ew
r
cv
dv
=-
×+
21
1
1
1
()
()i, (2)
vS S
12111
=+
,vS S
22111
=-
,
where wis the radian frequency, dis the thickness of a substrate and cis ligh tvelocity, v1and v2are
composite terms, which represent the addition and subtraction of S-parameters.
4. DESIGN AND RESULTS OF RMPA WITH DOUBLE H SHAPED METAMATERIAL
EMBEDDED BENEATH THE PATCH
The optimized double H shaped resonator has been located within the substrate at the height of 1.56 mm
from the ground (Fig. 7). Antenna resonates at 5.2 GHz with reflection coefficient of –21.99 dB and 220
MHz bandwidth (Fig. 8). Gain of metamaterial embedded patch antenna is 4.47 dB (Fig. 9), which is
approximately the same as gain of the reference antenna. By embedding metamaterial the reflection
coefficient decreases from –11.68 to –21.99 dB as compared to the reference antenna, because of better
impedance matching. The bandwidth increases from 70 to 220 MHz. The radiation patterns of metamaterial
embedded patch antenna in E-plane and H-plane are presented in Fig. 10. They are almost the same as
radiation patterns of the reference antenna (Fig. 4).
Embedding the double H shaped metamaterial in patch antenna is advantageous technique because it
provides improvement of return loss, enhancement of bandwidth, better impedance matching without
reduction of gain.
5. DESIGN AND RESULTS OF DOUBLE H SHAPED METAMATERIAL EMBEDDED RMPA
WITH SUPERSTRATE
To further increase the gain a superstrate of double H shaped resonator has been applied over the
metamaterial embedded patch antenna. From Fig. 6 we can see that the permittivity of resonator is close to
zero at the resonating frequency and, hence, the refractive index n=± emis also close to zero. Therefore, all
the rays coming from the antenna will be very close to normal to the surface and all the refracted rays will
RADIOELECTRONICS AND COMMUNICATIONS SYSTEMS Vol. 59 No. 11 2016
498 KAUR et al.
Fig. 5. Fig. 6.
L1
L2
W1
L3
123456 7f, GHz
20
10
0
–10
–20
–30
e,m
Permittivity
Permeability
propagate in almost the same direction around the normal and, consequently, the better gain and efficiency
can be achieved.
Figures 11 and 12 show the simulated and fabricated metamaterial embedded antenna with superstrate of
double H resonator. Resonant frequency of metamaterial embedded antenna does not change by adding the
superstrate (Fig. 13). The fabricated metamaterial embedded patch antenna with superstrate wass tested
using vector network analyzer. The measured and simulated results are in good agreement (Fig. 13).
The reflection coefficient S11 of fabricated RMPA was measured in anechoic chamber. Experimental and
simulated results are shown in Fig. 13. The gain of antenna increases from 4.48 to 6.72 dB due to the addition
of superstrate of metamaterial. The efficiency improves from 57.3 to 80.2%. The simulated and measured
RADIOELECTRONICS AND COMMUNICATIONS SYSTEMS Vol. 59 No. 11 2016
PERFORMANCE ENHANCEMENT OF RMPA USING DOUBLE H SHAPED METAMATERIAL 499
Fig. 7. Fig. 8.
Fig. 10.Fig. 9.
Fig. 11. Fig. 12.
02550mm
2 2.5 3 3.5 4 4.5 5 5.5 6 f, GHz
S11,dB
–5
–2.5
–7.5
–10
–12.5
–15
–17.5
–20
–22.5
2 2.5 3 3.5 4 4.5 5 5.5 6 f, GHz
Gain, dB
2.5
0
–2.5
–5
–7.5
–10
–60°
–90°
–120°
–150°
–180°
–30°
0°
30°
60°
90°
120°
150°
–7
–14
–21
–28
E-plane
H-plane
02550mm
radiation patterns of proposed RMPA in E- and H-planes are shown in Figs. 15, 16, respectively. Table 1
shows the comparison of performance parameters of the proposed RMPA with reference antenna.
RADIOELECTRONICS AND COMMUNICATIONS SYSTEMS Vol. 59 No. 11 2016
500 KAUR et al.
Table 1
Parameter Reference
RMPA
Double H
shaped
metamaterial
embedded
RMPA
RMPA with
embedded substrate
and superstrate of
double H
metamaterial
(proposed antenna)
Resonant frequency, GHz 5.2 5.1941 5.22
Return loss, dB –11.68 –21.99 –22.78
Bandwidth, MHz 70 220 220
Gain, dB 4.48 4.47 6.72
3 dB beamwidth (j= 0°), deg. 78.63 78.65 63.3
3 dB beamwidth (j= 90°), deg. 85.69 85.79 58.83
Radiation efficiency, % 57.3 57.2 80.2
Fig. 15. Fig. 16.
46810f, GHz 5 5.1 5.2 5.3 5.4 f, GHz
S11,dB
–25
–20
–15
–10
–5
Simulated
Measured
Gain, dB
5.2
5.6
6.0
6.4
6.8
Simulated
Measured
300°
270°
240°
210°
180°
330°
0°
30°
60°
90°
120°
150°
–25
–20
–15
–10
Simulated
Measured
–20
–15
–10
–5
0
–5
0
Fig. 13. Fig. 14.
300°
270°
240°
210°
180°
330°
0°
30°
60°
90°
120°
150°
–25
–20
–15
–10
Simulated
Measured
–20
–15
–10
–5
0
–5
0
–25
6. CONCLUSIONS
In this paper a high gain RMPA with good impedance matching and better bandwidth as compared to
reference antenna has been designed using DNG double H shaped metamaterial. The proposed antenna
improves the reflection coefficient from –11.68 to –22.78 dB. The efficiency has been improved from 57.3
to 80.2% with respect to the reference antenna. These improvements demonstrate the better impedance
matching of metamaterial embedded antenna as compared to the reference antenna.
The proposed antenna has 6.72 dB gain at resonance frequency and it is more directive than the reference
antenna. The bandwidth of metamaterial embedded antenna has been improved from 70 to 220 MHz.
Therefore, it can be concluded that the performance parameters of antenna, namely, its gain, reflection
coefficient, bandwidth, efficiency and directivity can be improved by proper designing and embedding of
metamaterial into the reference antenna.
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