Novel High-Gain Narrowband Waveguide-Fed Filtenna using Genetic Algorithm

International Journal of Electrical and Computer Engineering (IJECE)
Vol. 7, No. 1, February 2017, pp. 253~259
ISSN: 2088-8708, DOI: 10.11591/ijece.v7i1.pp253-259  253
Journal homepage: http://iaesjournal.com/online/index.php/IJECE
Novel High-Gain Narrowband Waveguide-Fed Filtenna using
Genetic Algorithm
Mahdi Ghorbani, Habib Ghorbaninejad
Department of Electrical Engineering, University of Guilan
Article Info ABSTRACT
Article history:
Received Sep 11, 2016
Revised Nov 27, 2016
Accepted Dec 18, 2016
Filtenna is an antenna with filtering feature. There are many ways to design a
filtenna. In this paper, a high-gain narrowband waveguide-fed aperture
filtenna has been proposed and designed. A patterned plane, which is
designed using genetic algorithm has been used at the open end of the
waveguide fed, mounted on a conducting ground plane. To design the
patterned pattern, magnetic field integral equation of the structure has been
derived, so it has been solved using method of moments. The proposed
filtenna has been simulated with HFSS that confirms the results obtained by
method of moments. Finally, an unprinted dielectric as a superstrate has been
used to enhance the gain of the filtenna. The filtenna bandwidth is 1.76%
(160 MHz) which has the gain of 15.91 dB at the central frequency
of 9.45 GHz.
Keyword:
Filtenna
Genetic algorithm
High gain
Method of moment
Narrow band Copyright © 2017 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Habib Ghorbaninejad,
Department of Electrical Engineering,
University of Guilan,
University of Guilan, Rasht, Guilan Province, Iran.
Email: ghorbaninejad@guilan.ac.ir
1. INTRODUCTION
In communication systems with sensitive receiver and transporter, it is necessary to filter the
unwanted signals. Often this unwanted signals are strong compared to the main signal and therefore it should
be eliminated. The best way for eliminating this unwanted signals is filtenna. Filtenna is a multifunction
device, which is done filtering feature and radiation at the same time. Therefore the main signal is protected.
There are many way for design of various type of filtenna with narrow or wideband application. Also many
technics is used for adjust bandpass and rejection band of filtering feature.
Microstrip antenna is one of the most attractive types of antennas. Microstrip antenna usually is used
in wideband application, but in some literature it is used in narrowband, or in multiband application. With an
umbrella shape radiation element, and modified ground plane, filtering feature can be achieved [1].
Increasing the number of resonant frequency can enhance the bandwidth of the filtenna [2]. In [3] wideband
microstrip antenna is used, and narrowband filtering feature is achieved with electronically adjusting of
resonant frequency. Also, defected ground plane [4], and H-shape slot on the microstrip [5] can create several
resonant frequency. The gain of the antenna is one of the most important factors in the design process, while
the mentioned antennas suffer from the deficiency of undesired gain in the frequency range.
Substrate integrated waveguide has also been used for filtenna design. In [6] horn antenna with FSS
is used with acceptable gain. Filtering feature can obtained through using coupled resonator, which the last
resonator also contains the radiating element [7]. Filtenna with balun and Yagi-Uda antenna as driven
elements has been investigated in [8], which have a low gain with complex configuration. Substrate
integrated waveguide base antenna is used for filtenna design [9].

 ISSN: 2088-8708
IJECE Vol. 7, No. 1, February 2017 : 253 – 259
254
In [10] filtenna is based on wideband coupled planar waveguide (CPW) antenna, which filtering
feature add rejection band to the antenna. This filtenna have a low gain. In [11] DRA multiband filtenna is
designed. In this paper three-segmental relatively low permittivity thin dielectric has been used and two metal
plates are applied to set four different frequency band. Also, planar phased-array antenna with frequency
selectivity properties has been investigated, so that filtering characteristic has been obtained in the common-
mode rejection module, consisting in a planar hybridring [12].
In this paper a novel filtenna is proposed. The filtenna is based on waveguide-fed aperture antenna.
For filtering feature, simple aperture is replaced by a patterned plane one which is mounted on the ground
plane. Green’s function of the form of magnetic field integral equations (MFIEs) in the waveguide is derived
and solved using method of moments. The desired patterned plane is obtained from genetic algorithm using
optimization. At the final step for the gain enhancement, unprinted high permittivity dielectric slabs are used
in front of the aperture as superstrate, based on Fabry-Perot theorem. The proposed filtenna has a good gain,
return loss at the operating frequency.
2. DESIGN METHOD OF THE PROPOSED STRUCTURE
2.1. The Proposed Filtenna Structure
The proposed antenna is based on waveguide-fed aperture antenna with patterned plane mounted on
a ground plane, along with two unprinted dielectric slabs (as superstrates) which are located over patterned
plane for gain improvement. Patterned plane is printed on a dielectric substrate. Figure 1 shows three
dimensional view of the proposed filtenna configuration. For this purpose WR90 waveguide with dimension
of 22.86×10.16 mm is selected. WR90 is used in X-band at 8-12 GHz. Substrate with low permittivity of 1.2
is selected. Figure 2 shows the side view of the proposed filtenna along with waveguide fed structure.
Figure 1. Three Dimensional View of the Proposed Filtenna Configuration
Figure 2. The Side View of the Proposed Filtenna along with Waveguide Fed Structure

IJECE ISSN: 2088-8708 
Novel High Gain Narrowband Waveguide Fed Filtenna Using Generic Algorithm (Mahdi Ghorbani)
255
2.2. Green’s Function and Magnetic Field Integral Equations (MFIEs)
At the first step in the design process, the desired pattern should be obtained. For this purpose, the
electric and magnetic field in the various regions, including substrate layer and hollow waveguide section is
written. Boundary conditions are applied at the common surface between substrate and air inside of the
waveguide, and between common surface between substrate and air out of the waveguide and the following
matrix equation is achieved.
[ ] [ ] * + (1)
where and are the magnetic fields in dielectric substrate in x and y direction respectively. and
are magnetic current in x and y direction respectively. , , and are green functions that are
given as the following:
(2)
(3)
(4)
where , , , are as follows:
(5)
(6)
√
(7)
√
(8)
where , are admittance of air and dielectric substrate in TM mode, respectively, and , are
admittance of air and dielectric substrate in TE mode, respectively. , , where a, b are
the WR90 dimensions and m, n, is non-negative integers due to propagating or evanescent modes.
To solve the obtained equations, unknown magnetic current and on the patterned plane
(corresponding to non-metallic parts of patterned plane) in the x and y direction is expanded in terms on sub
domain basis functions to apply method of moments, as follows:
∑ (9)
∑ (10)
[ ( | |)]
[ ]
(11)
[ ( | |)]
[ ]
(12)
The integral equation of magnetic field is solved using method of moment (Galerkin Method). This
result is used in MATLAB in genetic algorithm optimization to find the best pattern, which is match with
given specifications.

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256
2.3. Genetic Algorithm Optimization
Genetic algorithm is a useful way for complicated optimization. For example in [13], genetic
algorithm has been used in smart antenna for fast dynamically change of the environment. In this paper we
have used the genetic algorithm to match the return loss of the patterned plane with desired one.
Waveguide cross section is divided to 24*16 rectangular subsections. For a given patterned plane,
some of the subsections are metalized and the remained ones are non-metalized. The aim is to fine a
patterned plane with given specifications. Here, patterned plane has been considered to have symmetry in x,
y directions to reduce optimization time and computer memory; therefore just one quarter of waveguide cross
section, means, 12*8 subsections is used on genetic algorithm optimization. Then desired return loss of the
filtenna with that of a simple series LC circuit is matched to meet filtering feature.
2.4. The Proposed Filtenna Results
Figure 3 show the designed patterned plane obtained using genetic algorithm. The proposed
structure has been simulated with HFSS. Figure 4 show the return loss of the desired resonator compared
with that of the designed patterned plane. Resonant frequency of the desired resonator has been assumed 10
GHz, but the designed resonant frequency in HFSS simulation result is equal to 9.77 GHz.
Figure 3. The Patterned Plane Obtained using
Genetic Algorithm
Figure 4. Return loss of Desired Resonator Compared
with that of the Designed Patterned Plane
Figure 5a shows the return loss of the filtenna before and after locating of the patterned plane. It
shows the effect of the patterned plane. Fig. 5b is the gain of the filtenna before and after using patterned
plane and it shows that this patterned plane decrease the gain of the filtenna.
(a) (b)
Figure 5. (a) The return loss and (b) The Gain of the Proposed Filtenna before and after using Patterned Plane

IJECE ISSN: 2088-8708 
257
2.5. Gain Enhancement
Using Partially Reflecting Sheet (PRS) as superstrate in front of the aperture and parallel to the
ground plane at a suitable distance, it is possible to enhance the gain of this type of antennas. This introduced
first time with Trentini in 1956 [14]. This improvement is based on cavity model, which is created between
ground plane and superstrate. Beam is multi-reflected between these two planes, and leaked from superstrate
to the broadside. The maximum gain is obtained while maximum numbers of these beams are in same
direction.
(13)
( ) (14)
( ) (15)
where G is the gain, BW is the bandwidth, is the distance between ground plane and superstrate, ρ is the
reflection coefficient magnitude, λ is wavelength, and ψ0 is phase angle of the reflection coefficient.
Final configuration of this filtenna is composed of an aperture mounted on the center of conducting
ground plane, which is fed with waveguide. Two high permittivity dielectrics as superstrates are located in
front of the aperture at the given distance. Superstrates is assumed RO3010 with permittivity of 10.2.
Distance between ground plane and superstrate is approximately ≅λ/2 and =32.6 mm.
2.6. The structure design parameter
At this design, WR90 waveguide is used with dimension of 22.86×10.16 mm. The central frequency
of the proposed antenna is 9.45 GHz, corresponding to wavelength of 31.75mm. The dimension of each
section on the patterned aperture is 0.93×0.65 mm. The aperture located at the center of ground plane with
dimension of Xg=110 mm and Yg=75 mm (3.5λ×2.4λ). In front of the aperture two layers of superstrates is
used. Superstrates are unprinted dielectric and they are chosen RO3010 material with εr1=10.2, and they are
located at distance of =16.8 mm and =32.6 mm (0.53λ and 1.06λ) from the aperture. Dimension of both
superstrates are Xs=55.3 mm and Ys=37.9 mm (1.75λ×1.2λ) with thickness of Ts=2.0 mm. The patterned
plane is printed on a dielectric slab of thickness 0.5 mm. The electric permittivity constant of the substrate is
chosen εr2=1.2. The resonant frequency moves toward the lower frequency range when substrate permittivity
increases.
2.7. Final results of the proposed filtenna
This filtenna is simulated with HFSS and the following results obtained. The central frequency of
the proposed filtenna is 9.45 GHz with 1.76% bandwidth (160 MHz bandwidth, 9.37-9.54 GHz). Figure 6
shows the return loss and the gain of the proposed filtenna.
(a) (b)
Figure 6. (a) The return loss and (b) The gain of the proposed filtenn

 ISSN: 2088-8708
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It can be observed from Figure 6 that the proposed filtenna gain at the design frequency is 15.91 dB
so that significantly is improved compared with the case without superstrates. Radiation pattern of E-plane
and H-plane of the proposed filtenna are shown on Figure 7(a) and (b), respectively. Side lobe level and back
lobe level of the proposed filtenna are respectively 15.1dB and 19.0dB. Figure 8 shows three-dimensional
view of the gain in dB.
(a) (b)
Figure 7. (a) E-plane and (b) H-plane of the proposed Filtenna
Figure 8. 3-D polar view of the gain in dB
3. CONCLUSION
A novel waveguide fed aperture filtenna has been proposed. At this work, magnetic field integral
equations solved with galerkin’s method to obtain magnetic current density on the patterned aperture. The
optimized pattern on printed circuit board (PCB) is obtained using genetic algorithm. Finally the return loss
and the gain, has been enhanced using two superstrate and the ground plane.
This filtenna have 9.45 GHz center frequency with 1.76% bandwidth of 3dB and 15.91dB gain at
the centre frequency. In the proposed filtenna side lobe level and back lobe level are respectively 15.1dB and
19.0dB.
REFERENCES
[1] W. Rongda and G. Peng, “A compact Microstrip Ultra-wideband Filtenna,” 15th International conference on
electronic packaging technology, pp. 1353 – 1355, 2014.
[2] H. H. M. Ghouz, “New Compact Microstrip Patch Filtenna Structures with Partitioned Ground for 3G/4G
Applications,” International Journal of Engineering & Technology IJET-IJENS, vol/issue: 12(05), 2012.
[3] A. H. Ramadan, et al., “A Narrowband Frequency-Tunable Antenna for Cognitive Radio Applications,” 6th
European Conference on Antennas and Propagation (EUCAP), pp. 3273 – 3277, 2012.
[4] A. Zamanifekri, et al., “Dual-Frequency Filtenna Using Defected Ground Structure for VSAT Applications,”
Antennas and Propagation Society International Symposium (APSURSI), pp. 434 – 435, 2014.

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[5] R. H. Zaghloul and H. H. M. Ghouz, “A New Compact Multi Resonance H-Patch Filtenna,” Antennas and
Propagation Society International Symposium (APSURSI), pp. 1718 – 1719, 2013.
[6] G. Q. Luo, et al., “Filtenna Consisting of Horn Antenna and Substrate Integrated Waveguide Cavity FSS,” IEEE
Transactions on Antennas and Propagation, vol/issue: 55(1), 2007.
[7] O. A. Nova, et al., “Filter-Antenna Module Using Substrate Integrated Waveguide Cavities,” IEEE Antennas and
Wireless Propagation Letters, vol. 10, pp. 59 – 62, 2011.
[8] S. Yu, et al., “Integrated Millimeter Wave Filtenna for Q-LINKPAN Application,” 6th European Conference on
Antennas and Propagation (EUCAP), pp. 1333 – 1336, 2012.
[9] C. Yu, et al., “Ku-Band Linearly Polarized Omnidirectional Planar Filtenna,” IEEE Antennasand Wireless
Propagation Letters, vol. 11, 2012.
[10] Y. Jang, et al., “Compact Band-selective Filter and Antenna for UWB Application,” PIERS Online, vol/issue: 3(7),
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[11] H. Younesiraad, et al., “Small Multi-Band Rectangular Dielectric Resonator Antennas for Personal Communication
Devices,” International Journal of Electrical and Computer Engineering (IJECE), vol/issue: 4(1), pp. 1~6, 2014.
[12] L. Cifola, et al., “Compact Design of a Planar Filtering Antenna Array including a Frequency Selective Common-
Mode Rejection Module,” Antennas and Propagation Society International Symposium (APSURSI), pp. 1-2, 2012.
[13] J. R. Mohammad, “Comparative Performance Investigations of Stochastic and Genetic Algorithms Under Fast
Dynamically Changing Environment in Smart Antennas,” International Journal of Electrical and Computer
Engineering (IJECE), vol/issue: 2(1), pp. 98~105, 2012.
[14] G. V. Trentini, “Partially reflecting sheet array,” IRE Trans. Antennas Propagat., vol. 4, pp. 666-671, 1956.
BIOGRAPHIES OF AUTHORS
M. Ghorbani received B.Sc. degree in Electrical Engineering from Isfahan University of
Technology (IUT), Isfahan, Iran in 2003. He work 10 years in industry as a design and R&D
manager. He received M.Sc. degree in 2016 in Fields and Wave Communication Engineering
from University of Guilan.
H. Ghorbaninejad received B. Sc. degree from University of Guilan in 2003 and M. Sc. and Ph.
D. degrees from Iran University of Science and Technology (IUST) in 2005 and 2010
respectively, all in Fields and Wave Communication Engineering. He is currently assistant
professor at Department of Electrical Engineering of University of Guilan. His scientific fields of
interest are electromagnetic problems including microwave filter design, compact microwave
devices and Green’s function of microwave structures.

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