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TELKOMNIKA, Vol.17, No.4, August 2019, pp.1663~1669
ISSN: 1693-6930, accredited First Grade by Kemenristekdikti, Decree No: 21/E/KPT/2018
DOI: 10.12928/TELKOMNIKA.v17i4.12764  1663
Received July 10, 2018; Revised January 26, 2019; Accepted March 14, 2019
Wide to multiband elliptical monopole reconfigurable
antenna for multimode systems applications
I. H. Idris*1
, M. R. Hamid2
, K. Kamardin3
, M. K. A. Rahim4
1,2,4
Advanced RF and Microwave Research Group (ARFMRG), School of Electrical Engineering, Faculty
Engineering, Engineering, Universiti Teknologi Malaysia, UTM Johor Bahru, 81310 Johor, Malaysia
3
Department of Electronic Systems Engineering, Malaysia–Japan International Institute of Technology
(MJIIT), Universiti Teknologi Malaysia, 54100 Kuala Lumpur, Malaysia
3
Wireless Communication Centre (WCC), Universiti Teknologi Malaysia, 54100 Kuala Lumpur, Malaysia
*Corresponding author, e-mail: husnaidris89@gmail.com
Abstract
Wideband-multiband reconfigurable elliptical monopole antenna is investigated in this paper.
By having conventional elliptical monopole antenna, wideband operating frequency is obtained.
With the combination of dual pairs of slotted arms and a band-pass filter on the ground plane of the elliptical
monopole, multiband is achieved. Dual-band operating frequencies at 1.6 GHz and 2.6 GHz while wideband
operates from 3.35 GHz to 9 GHz. Therefore, wide range of wireless communication systems is obtained
from the proposed antenna to support the multiband mode (i.e. GPS and LTE) and UWB systems. Frequency
reconfigurable is achieved by controlling the switches integrated on the antenna structure. Simulated results
of reflection coefficient, radiation patterns and gain performance are presented. The proposed antenna
design is suitable candidate for different wireless communication applications.
Keywords: band-pass filter, multiband antenna, reconfigurable, wideband antenna
Copyright © 2019 Universitas Ahmad Dahlan. All rights reserved.
1. Introduction
Reconfigurable antennas are still attracting the interest of many researchers in recent
years. This is because these antennas give many benefits to improve the performance of RF
front ends. Unlike conventional antennas [1-8] which has a fixed operating frequency or pattern
types, reconfigurable antennas have the ability to varying its operating frequencies and also
radiation pattern to satisfy the modern communication systems. Most of the antennas in [1-4]
have a wideband operating frequency, using a mictrostrip patch antenna design to operate in
Ultra-wide band (UWB) frequency range. Meanwhile, reported antennas in [5-8] only can
operate in multiband frequency. Despite of having compact size of antennas, they did not have
the ability to control the operating frequencies compared to reconfigurable antennas.
Reconfigurable antennas can have frequencies switching or tuning [9-19] and also
changing its radiation pattern or beam steering [20-23]. Most of the reconfigurable antennas can
be used in cognitive radio systems, where most of them are having wideband to narrowband
reconfiguration. However, having only one frequency operating at one time, will restraint
the antenna to function for different applications simultaneously. More functionality such as
wideband to narrowband and multiband reconfiguration can be more suitable to serve in
the rapid growth of communication systems nowadays.
Most antennas reported to work on narrowband to narrowband [9,10] and wideband to
narrowband reconfigurations such as in [11,12]. There are also reported antennas that can
reconfigure between wideband to multiband [13], multiband to another multiband [14,15] and
multiband to narrowband [16-19] operating frequencies. Lately, single to dual and triple-band
reconfigurations have been getting much interest from researchers. Some reported antennas
in [18, 19] are able to switch their operating frequencies using a simple structure antenna
design. Antenna in [18] using slotted bowtie antenna and two pairs of slot in the ground plane to
create additional bands. Circular slotted with different radii is presented in [19] to have a
different operating frequency when the switches are turned ON or OFF. Both of the antennas
can work from 2.0 GHz to 7.0 GHz.
The best way to bias the switches are to have circuit simplicity, which means no via will
be involved [14]. Thus, monopole antenna with coplanar waveguide (CPW)-feedline is a suitable
 ISSN: 1693-6930
TELKOMNIKA Vol. 17, No. 4, August 2019: 1663-1669
1664
solution to provide wideband operating frequency. In this paper, elliptical monopole antenna is
chosen to become wideband radiator, integrated with the dual-pairs of slotted arm located at
the ground plane to produce the multiband mode. In order to eliminate the harmonic frequency,
produce by multiband radiator, band-pass filter is incorporated.
The antenna can operate at 1.6 GHz and 2.6 GHz in multiband mode while in wideband
mode, the antenna can operate from 3.3 GHz to 9.0 GHz. Unlike antenna mentioned in [24],
the antenna can only cover frequency range from 2.0 GHz to 6.0 GHz for both multiband and
wideband mode. In other words, multiband operating frequency of antenna in [24], is within
the wideband operating frequency too. However, the multiband operating frequency of
the proposed antenna, is outside of the wideband operating frequency. Therefore, the proposed
antenna in this paper can cover wider range of frequencies compared to antenna in [24]. Details
of the antenna structure is explained in Section 2. The antenna performances including
reflection coefficient, radiation pattern and gain are presented in section 3. lastly, this paper is
concluded in section 4.
2. Antenna Structure
The design and simulation process are performed using CST® software. Initial antenna
structure, will be called as antenna A, is shown in Figure 1 (a) while the band-pass filter consists
of four stubs is shown in Figure 1 (b). Antenna A consists of elliptical monopole radiator, have
a semimajor of A value and semiminor of B value, is fed by a CPW-feedline to produce
wideband mode. Dual pairs of slot dipole arms (arm1 and arm2) together with rectangular box
(boxR) is located in the ground plane to fully utilised the wideband antenna. In order to produce
the multiband mode, the length of arm1 and arm2 are approximately quarter of wavelength of
1.6 GHz and 2.6 GHz, respectively. Wideband antenna is ranging from 3 GHz to 9 GHz while
dual band antenna operates at 1.6 GHz and 2.6 GHz. The simulated reflection coefficient (S11)
results are shown in Figure 2 (a).
Band-pass filter as shown in Figure 1 (b) consists of four pairs of rectangular stubs.
Two rectangular stubs are connected with one connecting part to reduce the number of
switches. Parametric studies of this band-pass filter is presented in [25]. It produces pass band
from 1.38 GHz to 3.29 GHz and stop band from 3.29 GHz to 9.0 GHz as shown in Figure 2 (b).
By integrating the band-pass filter into the antenna structure, the filter will be able to eliminate
the harmonic frequencies created by antenna A in the multiband mode.
Figure 3 illustrates the proposed antenna structure with the combination of antenna A
and band-pass filter. The proposed antenna will later be called as antenna B. Antenna B using
FR-4 substrate with a relative dielectric constant of 4.3 and thickness of 1.6 mm. The antenna
consists of four pairs of switches. Two switches denoted as SW1 while the remaining switches
are called as SW2. In this paper, ideal switch is used to achieve antenna reconfigurability.
By switching ON SW1 and SW2 is turned OFF, multiband mode is achieved. In order to get
wideband mode, SW1 needs to be turned OFF and SW2 is switched ON. Switch ON means
copper strip is present while switch OFF means vacuum block is used to replace the copper
strip. Table 1 represents the value of parameters used in designing the proposed antenna.
Others parameters which are not shown here can be refered at [24].
SW1 SW2
(a)
stub4
stub3
stub2
stub1
stub4
stub3
stub2
stub1
Port 2
Port 1
(b)
Figure 1. The structure of (a) Antenna A (b) band-pass filter [25]
TELKOMNIKA ISSN: 1693-6930 
Wide to multiband elliptical monopole reconfigurable antenna... (I. H. Idris)
1665
S11 antOnly
Frequency, GHz
1 2 3 4 5 6 7 8 9
S11,dB
-40
-30
-20
-10
0
multiband mode
wideband mode
(a)
Frequency, GHz
1 2 3 4 5 6 7 8 9
S11/S21,dB
-40
-30
-20
-10
0
S11
S21
(b)
Figure 2. Simulated results of (a) S11 of antenna A (b) S11 and S21 of band-pass filter
stub1
stub2
stub3
stub4
arm1
arm2
A
B
l
w
boxR
SW1 SW2
Figure 3. The proposed antenna B
Table 1. Parameters of the Proposed
Antenna B Structure
Parameter
Dimension
(mm)
Parameter
Dimension
(mm)
l 115 boxR 30
w 62 stub1 40
A 7 stub2 9
B 4 stub3 7
arm1 24 stub4 6
arm2 16
3. Results and Analysis
Figure 4 shows the reflection coefficient (S11) in the multiband and the wideband modes.
In the multiband mode, harmonic frequencies of antenna B is completely eliminated from
3.0 GHz to 6.0 GHz as opposed to antenna A. In the wideband mode, it shows that the result of
antenna B is almost similar to antenna A even after adding the filter. The proposed antenna is
simulated results of S11 for multiband and wideband modes are shown in Figure 5. Dual-band is
achieved at 1.6 GHz and 2.6 GHz with S11 value of -19.67 dB and -14.33 dB. The bandwidth of
lower band (1.6 GHz) is 280 MHz, range from 1.51 GHz to 1.79 GHz. While upper band
bandwidth of 140 MHz, which is ranging from 2.49 GHz to 2.63 GHz, is achieved. However,
there is another unwanted harmonic appears at 8.2 GHz with S11 value of -11.00 dB. Such result
may occur because of the S11 result of the band-pass filter is below -3 dB from 7 GHz until 9 GHz
as shown in Figure 2 (b). Therefore, the filter does affect the proposed antenna result from 7 GHz
to 9 GHz in the multiband mode. Further analysis of this problem will be explained in simulated
gain result. It can be noticed in wideband mode that the antenna can operate well from 3.35 GHz
to 9 GHz. Three peaks are noticeable with the value of S11 below than -9 dB, therefore it is
acceptable to be counted as a wideband from 3.35 GHz to 9 GHz.
Simulated radiation pattern results are shown in Figure 6. The radiation patterns
simulated at 1.6 GHz and 2.6 GHz in multiband mode while 3.5 GHz and 5.2 GHz in wideband
mode. H-plane for both multiband and wideband mode show that the patterns are nearly
omnidirectional over the operating frequencies. Bidirectional patterns are achived for both
modes of E-plane. The radiation patterns are almost uniform through out the entire bands either
in multiband or wideband mode. Radiation pattern at 5.2 GHz for wideband mode as shown in
Figure 6 (d) is slightly different compared to others bands, but it has same radiation pattern with
or without filter as shown in Figure 7 (d). Figure 7 shows simulated radiation pattern for
multiband and wideband mode of antenna A. It can be noticed that the similar patterns are
obtained at same frequency between Figure 6 and Figure 7.
 ISSN: 1693-6930
TELKOMNIKA Vol. 17, No. 4, August 2019: 1663-1669
1666 S11 multiband
simulated result
Frequency, GHz
1 2 3 4 5 6 7 8 9
S11,dB
-40
-30
-20
-10
0
antenna A
antenna B
(a)
S11 wideband
simulated result
Frequency, GHz
1 2 3 4 5 6 7 8 9
S11,dB
-40
-30
-20
-10
0
antenna A
antenna B
(b)
Figure 4. Simulated S11 results (a) multiband mode (b) wideband modeS11 ant+stub
simulated result
Frequency, GHz
1 2 3 4 5 6 7 8 9
S11,dB
-40
-30
-20
-10
0
multiband mode
wideband mode
Figure 5. Simulated S11 results of the proposed antenna (antenna B)
Figure 8 (a) shows the antenna structure of wideband mode without the multiband
resonator. Simulated radiation patterns of the antenna structure in Figure 8 (a) are shown in
Figures 8 (b)-(c). Only radiation patterns results were shown here to show the consistency
results of the radiation pattern in wideband mode between Figure 1 (a), Figure 3 and
Figure 8 (a). From the figures, it can be noticed that radiation patterns from Figure 8 (b)-(c) are
almost same with the patterns in Figure 6 (c)-(d) and Figure 7 (c)-(d). Consistency in the
radiation pattern results are achieved; between the antenna structures in Figure 8 (a),
Figure 1 (a) and Figure 3. Therefore, the radiation patterns are unchanged and followed the
frequency reconfigurable antenna concept, where the radiation patterns remain unchanged
even when the antenna is changed to different states or modes.
The simulated gain versus reflection coefficient results can be viewed in Figure 9.
In multiband mode, maximum gain can be obtained at 1.6 GHz and 2.6 GHz, where the
reflection coefficient (S11) is below than -10 dB as expected. However, at 8.2 GHz (-11.0 dB),
the maximum gain value of 0.32 dBi is obtained. In addition, higher gains which are 3.29 dBi
and 2.64 dBi can be seen at 7.2 GHz and 8.7 GHz, respectively. But, the reflection coefficient
value is only -3.9 dB at both of frequencies, 7.2 GHz and 8.7 GHz. In this case, only almost 60%
power will be transmitted where 40% left will be reflected back to the source. Therefore, we are
going to neglect the value because it will produce a lot of losses while transmitting the data. In
Figure 9 (b), wideband gain result is higher than 2.1 dBi is recorded for the entire bands, from
3.5 GHz to 9.0 GHz. The maximum gain value of 5.54 dBi can be seen at 6.8 GHz. The overall
result of gain for wideband mode is in good performance through out the frequency range from
3 GHz to 9 GHz. The summary of simulated gain results is tabulated in Table 2.
TELKOMNIKA ISSN: 1693-6930 
Wide to multiband elliptical monopole reconfigurable antenna... (I. H. Idris)
1667
Multiband mode
1.6 GHz
-40
-20
0
0
30
60
90
120
150
180
210
240
270
300
330
H-plane
E-plane
Multiband mode
2.6 GHz
-40
-20
0
0
30
60
90
120
150
180
210
240
270
300
330
H-plane
E-plane
(a) (b)Wideband mode
3.5 GHz
-40
-20
0
0
30
60
90
120
150
180
210
240
270
300
330
H-plane
E-plane
Wideband mode
5.2 GHz
-40
-20
0
0
30
60
90
120
150
180
210
240
270
300
330
H-plane
E-plane
(c) (d)
Figure 6. Simulated radiation pattern results of antenna B; in multiband mode at
(a) 1.6 GHz (b) 2.6 GHz; in wideband mode at (c) 3.5 GHz (d) 5.2 GHz
-40
-20
0
0
30
60
90
120
150
180
210
240
270
300
330
-40
-20
0
0
30
60
90
120
150
180
210
240
270
300
330
-40
-20
0
0
30
60
90
120
150
180
210
240
270
300
330
-40
-20
0
0
30
60
90
120
150
180
210
240
270
300
330
(a) (b) (c) (d)
Figure 7. Simulated radiation pattern results of antenna A; in multiband mode at
(a) 1.6 GHz (b) 2.6 GHz; in wideband mode at (c) 3.5 GHz
(d) 5.2 GHz (solid line: H-plane, dashed line: E-plane)
Table 2. Simulated Gain Results
Multiband mode Wideband mode
Frequency (GHz) Gain (dBi) Frequency (GHz) Gain (dBi)
1.6 4.11 3.5 2.69
2.6 5.63 5.2 2.70
 ISSN: 1693-6930
TELKOMNIKA Vol. 17, No. 4, August 2019: 1663-1669
1668
(a)
-40
-20
0
0
30
60
90
120
150
180
210
240
270
300
330
(b)
-40
-20
0
0
30
60
90
120
150
180
210
240
270
300
330
(c)
Figure 8. (a) Wideband antenna structure without multiband resonator;
Simulated radiation pattern results in wideband mode at (b) 3.5 GHz (c) 5.2 GHz
(solid line: H-plane, dashed line: E-plane)S11 & gain ant+stub MULTIBAND
simulated result
Frequency, GHz
1 2 3 4 5 6 7 8 9
S11
,dB
-40
-30
-20
-10
0
10
Gain,dBi
-40
-30
-20
-10
0
10
S11
gain
(a)
S11 & gain ant+stub WIDEBAND
simulated result
Frequency, GHz
1 2 3 4 5 6 7 8 9
S11
,dB
-40
-30
-20
-10
0
10
Gain,dBi
-40
-30
-20
-10
0
10
S11
gain
(b)
Figure 9. Simulated gain and S11 results (a) multiband mode (b) wideband mode
4. Conclusion
A reconfigurable antenna using ideal switches has been designed and simulated in this
paper. Reconfigurability is achieved by switching ON or OFF four pairs of switches. Dual-band
resonance of 1.6 GHz and 2.6 GHz is obtained in multiband mode while the wideband mode is
ranging from 3.35 GHz to 9.0 GHz. Ideal switches will be replaced with real swiches such as
pin-diode, which determine that this antenna can work in actual environment. The proposed
antenna is suitable to be used in GPS, LTE and wideband wireless communication applications.
Acknowledgements
The authors would like to acknowledge the Ministry of Education (MoE) Malaysia,
Universiti Teknologi Malaysia (UTM) under the research grants (Vote No: 14J18 and 15H97)
and Advanced RF and Microwave Research Group (ARFMRG) for supporting this work.
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Wide to multiband elliptical monopole reconfigurable antenna for multimode systems applications

  • 1. TELKOMNIKA, Vol.17, No.4, August 2019, pp.1663~1669 ISSN: 1693-6930, accredited First Grade by Kemenristekdikti, Decree No: 21/E/KPT/2018 DOI: 10.12928/TELKOMNIKA.v17i4.12764  1663 Received July 10, 2018; Revised January 26, 2019; Accepted March 14, 2019 Wide to multiband elliptical monopole reconfigurable antenna for multimode systems applications I. H. Idris*1 , M. R. Hamid2 , K. Kamardin3 , M. K. A. Rahim4 1,2,4 Advanced RF and Microwave Research Group (ARFMRG), School of Electrical Engineering, Faculty Engineering, Engineering, Universiti Teknologi Malaysia, UTM Johor Bahru, 81310 Johor, Malaysia 3 Department of Electronic Systems Engineering, Malaysia–Japan International Institute of Technology (MJIIT), Universiti Teknologi Malaysia, 54100 Kuala Lumpur, Malaysia 3 Wireless Communication Centre (WCC), Universiti Teknologi Malaysia, 54100 Kuala Lumpur, Malaysia *Corresponding author, e-mail: husnaidris89@gmail.com Abstract Wideband-multiband reconfigurable elliptical monopole antenna is investigated in this paper. By having conventional elliptical monopole antenna, wideband operating frequency is obtained. With the combination of dual pairs of slotted arms and a band-pass filter on the ground plane of the elliptical monopole, multiband is achieved. Dual-band operating frequencies at 1.6 GHz and 2.6 GHz while wideband operates from 3.35 GHz to 9 GHz. Therefore, wide range of wireless communication systems is obtained from the proposed antenna to support the multiband mode (i.e. GPS and LTE) and UWB systems. Frequency reconfigurable is achieved by controlling the switches integrated on the antenna structure. Simulated results of reflection coefficient, radiation patterns and gain performance are presented. The proposed antenna design is suitable candidate for different wireless communication applications. Keywords: band-pass filter, multiband antenna, reconfigurable, wideband antenna Copyright © 2019 Universitas Ahmad Dahlan. All rights reserved. 1. Introduction Reconfigurable antennas are still attracting the interest of many researchers in recent years. This is because these antennas give many benefits to improve the performance of RF front ends. Unlike conventional antennas [1-8] which has a fixed operating frequency or pattern types, reconfigurable antennas have the ability to varying its operating frequencies and also radiation pattern to satisfy the modern communication systems. Most of the antennas in [1-4] have a wideband operating frequency, using a mictrostrip patch antenna design to operate in Ultra-wide band (UWB) frequency range. Meanwhile, reported antennas in [5-8] only can operate in multiband frequency. Despite of having compact size of antennas, they did not have the ability to control the operating frequencies compared to reconfigurable antennas. Reconfigurable antennas can have frequencies switching or tuning [9-19] and also changing its radiation pattern or beam steering [20-23]. Most of the reconfigurable antennas can be used in cognitive radio systems, where most of them are having wideband to narrowband reconfiguration. However, having only one frequency operating at one time, will restraint the antenna to function for different applications simultaneously. More functionality such as wideband to narrowband and multiband reconfiguration can be more suitable to serve in the rapid growth of communication systems nowadays. Most antennas reported to work on narrowband to narrowband [9,10] and wideband to narrowband reconfigurations such as in [11,12]. There are also reported antennas that can reconfigure between wideband to multiband [13], multiband to another multiband [14,15] and multiband to narrowband [16-19] operating frequencies. Lately, single to dual and triple-band reconfigurations have been getting much interest from researchers. Some reported antennas in [18, 19] are able to switch their operating frequencies using a simple structure antenna design. Antenna in [18] using slotted bowtie antenna and two pairs of slot in the ground plane to create additional bands. Circular slotted with different radii is presented in [19] to have a different operating frequency when the switches are turned ON or OFF. Both of the antennas can work from 2.0 GHz to 7.0 GHz. The best way to bias the switches are to have circuit simplicity, which means no via will be involved [14]. Thus, monopole antenna with coplanar waveguide (CPW)-feedline is a suitable
  • 2.  ISSN: 1693-6930 TELKOMNIKA Vol. 17, No. 4, August 2019: 1663-1669 1664 solution to provide wideband operating frequency. In this paper, elliptical monopole antenna is chosen to become wideband radiator, integrated with the dual-pairs of slotted arm located at the ground plane to produce the multiband mode. In order to eliminate the harmonic frequency, produce by multiband radiator, band-pass filter is incorporated. The antenna can operate at 1.6 GHz and 2.6 GHz in multiband mode while in wideband mode, the antenna can operate from 3.3 GHz to 9.0 GHz. Unlike antenna mentioned in [24], the antenna can only cover frequency range from 2.0 GHz to 6.0 GHz for both multiband and wideband mode. In other words, multiband operating frequency of antenna in [24], is within the wideband operating frequency too. However, the multiband operating frequency of the proposed antenna, is outside of the wideband operating frequency. Therefore, the proposed antenna in this paper can cover wider range of frequencies compared to antenna in [24]. Details of the antenna structure is explained in Section 2. The antenna performances including reflection coefficient, radiation pattern and gain are presented in section 3. lastly, this paper is concluded in section 4. 2. Antenna Structure The design and simulation process are performed using CST® software. Initial antenna structure, will be called as antenna A, is shown in Figure 1 (a) while the band-pass filter consists of four stubs is shown in Figure 1 (b). Antenna A consists of elliptical monopole radiator, have a semimajor of A value and semiminor of B value, is fed by a CPW-feedline to produce wideband mode. Dual pairs of slot dipole arms (arm1 and arm2) together with rectangular box (boxR) is located in the ground plane to fully utilised the wideband antenna. In order to produce the multiband mode, the length of arm1 and arm2 are approximately quarter of wavelength of 1.6 GHz and 2.6 GHz, respectively. Wideband antenna is ranging from 3 GHz to 9 GHz while dual band antenna operates at 1.6 GHz and 2.6 GHz. The simulated reflection coefficient (S11) results are shown in Figure 2 (a). Band-pass filter as shown in Figure 1 (b) consists of four pairs of rectangular stubs. Two rectangular stubs are connected with one connecting part to reduce the number of switches. Parametric studies of this band-pass filter is presented in [25]. It produces pass band from 1.38 GHz to 3.29 GHz and stop band from 3.29 GHz to 9.0 GHz as shown in Figure 2 (b). By integrating the band-pass filter into the antenna structure, the filter will be able to eliminate the harmonic frequencies created by antenna A in the multiband mode. Figure 3 illustrates the proposed antenna structure with the combination of antenna A and band-pass filter. The proposed antenna will later be called as antenna B. Antenna B using FR-4 substrate with a relative dielectric constant of 4.3 and thickness of 1.6 mm. The antenna consists of four pairs of switches. Two switches denoted as SW1 while the remaining switches are called as SW2. In this paper, ideal switch is used to achieve antenna reconfigurability. By switching ON SW1 and SW2 is turned OFF, multiband mode is achieved. In order to get wideband mode, SW1 needs to be turned OFF and SW2 is switched ON. Switch ON means copper strip is present while switch OFF means vacuum block is used to replace the copper strip. Table 1 represents the value of parameters used in designing the proposed antenna. Others parameters which are not shown here can be refered at [24]. SW1 SW2 (a) stub4 stub3 stub2 stub1 stub4 stub3 stub2 stub1 Port 2 Port 1 (b) Figure 1. The structure of (a) Antenna A (b) band-pass filter [25]
  • 3. TELKOMNIKA ISSN: 1693-6930  Wide to multiband elliptical monopole reconfigurable antenna... (I. H. Idris) 1665 S11 antOnly Frequency, GHz 1 2 3 4 5 6 7 8 9 S11,dB -40 -30 -20 -10 0 multiband mode wideband mode (a) Frequency, GHz 1 2 3 4 5 6 7 8 9 S11/S21,dB -40 -30 -20 -10 0 S11 S21 (b) Figure 2. Simulated results of (a) S11 of antenna A (b) S11 and S21 of band-pass filter stub1 stub2 stub3 stub4 arm1 arm2 A B l w boxR SW1 SW2 Figure 3. The proposed antenna B Table 1. Parameters of the Proposed Antenna B Structure Parameter Dimension (mm) Parameter Dimension (mm) l 115 boxR 30 w 62 stub1 40 A 7 stub2 9 B 4 stub3 7 arm1 24 stub4 6 arm2 16 3. Results and Analysis Figure 4 shows the reflection coefficient (S11) in the multiband and the wideband modes. In the multiband mode, harmonic frequencies of antenna B is completely eliminated from 3.0 GHz to 6.0 GHz as opposed to antenna A. In the wideband mode, it shows that the result of antenna B is almost similar to antenna A even after adding the filter. The proposed antenna is simulated results of S11 for multiband and wideband modes are shown in Figure 5. Dual-band is achieved at 1.6 GHz and 2.6 GHz with S11 value of -19.67 dB and -14.33 dB. The bandwidth of lower band (1.6 GHz) is 280 MHz, range from 1.51 GHz to 1.79 GHz. While upper band bandwidth of 140 MHz, which is ranging from 2.49 GHz to 2.63 GHz, is achieved. However, there is another unwanted harmonic appears at 8.2 GHz with S11 value of -11.00 dB. Such result may occur because of the S11 result of the band-pass filter is below -3 dB from 7 GHz until 9 GHz as shown in Figure 2 (b). Therefore, the filter does affect the proposed antenna result from 7 GHz to 9 GHz in the multiband mode. Further analysis of this problem will be explained in simulated gain result. It can be noticed in wideband mode that the antenna can operate well from 3.35 GHz to 9 GHz. Three peaks are noticeable with the value of S11 below than -9 dB, therefore it is acceptable to be counted as a wideband from 3.35 GHz to 9 GHz. Simulated radiation pattern results are shown in Figure 6. The radiation patterns simulated at 1.6 GHz and 2.6 GHz in multiband mode while 3.5 GHz and 5.2 GHz in wideband mode. H-plane for both multiband and wideband mode show that the patterns are nearly omnidirectional over the operating frequencies. Bidirectional patterns are achived for both modes of E-plane. The radiation patterns are almost uniform through out the entire bands either in multiband or wideband mode. Radiation pattern at 5.2 GHz for wideband mode as shown in Figure 6 (d) is slightly different compared to others bands, but it has same radiation pattern with or without filter as shown in Figure 7 (d). Figure 7 shows simulated radiation pattern for multiband and wideband mode of antenna A. It can be noticed that the similar patterns are obtained at same frequency between Figure 6 and Figure 7.
  • 4.  ISSN: 1693-6930 TELKOMNIKA Vol. 17, No. 4, August 2019: 1663-1669 1666 S11 multiband simulated result Frequency, GHz 1 2 3 4 5 6 7 8 9 S11,dB -40 -30 -20 -10 0 antenna A antenna B (a) S11 wideband simulated result Frequency, GHz 1 2 3 4 5 6 7 8 9 S11,dB -40 -30 -20 -10 0 antenna A antenna B (b) Figure 4. Simulated S11 results (a) multiband mode (b) wideband modeS11 ant+stub simulated result Frequency, GHz 1 2 3 4 5 6 7 8 9 S11,dB -40 -30 -20 -10 0 multiband mode wideband mode Figure 5. Simulated S11 results of the proposed antenna (antenna B) Figure 8 (a) shows the antenna structure of wideband mode without the multiband resonator. Simulated radiation patterns of the antenna structure in Figure 8 (a) are shown in Figures 8 (b)-(c). Only radiation patterns results were shown here to show the consistency results of the radiation pattern in wideband mode between Figure 1 (a), Figure 3 and Figure 8 (a). From the figures, it can be noticed that radiation patterns from Figure 8 (b)-(c) are almost same with the patterns in Figure 6 (c)-(d) and Figure 7 (c)-(d). Consistency in the radiation pattern results are achieved; between the antenna structures in Figure 8 (a), Figure 1 (a) and Figure 3. Therefore, the radiation patterns are unchanged and followed the frequency reconfigurable antenna concept, where the radiation patterns remain unchanged even when the antenna is changed to different states or modes. The simulated gain versus reflection coefficient results can be viewed in Figure 9. In multiband mode, maximum gain can be obtained at 1.6 GHz and 2.6 GHz, where the reflection coefficient (S11) is below than -10 dB as expected. However, at 8.2 GHz (-11.0 dB), the maximum gain value of 0.32 dBi is obtained. In addition, higher gains which are 3.29 dBi and 2.64 dBi can be seen at 7.2 GHz and 8.7 GHz, respectively. But, the reflection coefficient value is only -3.9 dB at both of frequencies, 7.2 GHz and 8.7 GHz. In this case, only almost 60% power will be transmitted where 40% left will be reflected back to the source. Therefore, we are going to neglect the value because it will produce a lot of losses while transmitting the data. In Figure 9 (b), wideband gain result is higher than 2.1 dBi is recorded for the entire bands, from 3.5 GHz to 9.0 GHz. The maximum gain value of 5.54 dBi can be seen at 6.8 GHz. The overall result of gain for wideband mode is in good performance through out the frequency range from 3 GHz to 9 GHz. The summary of simulated gain results is tabulated in Table 2.
  • 5. TELKOMNIKA ISSN: 1693-6930  Wide to multiband elliptical monopole reconfigurable antenna... (I. H. Idris) 1667 Multiband mode 1.6 GHz -40 -20 0 0 30 60 90 120 150 180 210 240 270 300 330 H-plane E-plane Multiband mode 2.6 GHz -40 -20 0 0 30 60 90 120 150 180 210 240 270 300 330 H-plane E-plane (a) (b)Wideband mode 3.5 GHz -40 -20 0 0 30 60 90 120 150 180 210 240 270 300 330 H-plane E-plane Wideband mode 5.2 GHz -40 -20 0 0 30 60 90 120 150 180 210 240 270 300 330 H-plane E-plane (c) (d) Figure 6. Simulated radiation pattern results of antenna B; in multiband mode at (a) 1.6 GHz (b) 2.6 GHz; in wideband mode at (c) 3.5 GHz (d) 5.2 GHz -40 -20 0 0 30 60 90 120 150 180 210 240 270 300 330 -40 -20 0 0 30 60 90 120 150 180 210 240 270 300 330 -40 -20 0 0 30 60 90 120 150 180 210 240 270 300 330 -40 -20 0 0 30 60 90 120 150 180 210 240 270 300 330 (a) (b) (c) (d) Figure 7. Simulated radiation pattern results of antenna A; in multiband mode at (a) 1.6 GHz (b) 2.6 GHz; in wideband mode at (c) 3.5 GHz (d) 5.2 GHz (solid line: H-plane, dashed line: E-plane) Table 2. Simulated Gain Results Multiband mode Wideband mode Frequency (GHz) Gain (dBi) Frequency (GHz) Gain (dBi) 1.6 4.11 3.5 2.69 2.6 5.63 5.2 2.70
  • 6.  ISSN: 1693-6930 TELKOMNIKA Vol. 17, No. 4, August 2019: 1663-1669 1668 (a) -40 -20 0 0 30 60 90 120 150 180 210 240 270 300 330 (b) -40 -20 0 0 30 60 90 120 150 180 210 240 270 300 330 (c) Figure 8. (a) Wideband antenna structure without multiband resonator; Simulated radiation pattern results in wideband mode at (b) 3.5 GHz (c) 5.2 GHz (solid line: H-plane, dashed line: E-plane)S11 & gain ant+stub MULTIBAND simulated result Frequency, GHz 1 2 3 4 5 6 7 8 9 S11 ,dB -40 -30 -20 -10 0 10 Gain,dBi -40 -30 -20 -10 0 10 S11 gain (a) S11 & gain ant+stub WIDEBAND simulated result Frequency, GHz 1 2 3 4 5 6 7 8 9 S11 ,dB -40 -30 -20 -10 0 10 Gain,dBi -40 -30 -20 -10 0 10 S11 gain (b) Figure 9. Simulated gain and S11 results (a) multiband mode (b) wideband mode 4. Conclusion A reconfigurable antenna using ideal switches has been designed and simulated in this paper. Reconfigurability is achieved by switching ON or OFF four pairs of switches. Dual-band resonance of 1.6 GHz and 2.6 GHz is obtained in multiband mode while the wideband mode is ranging from 3.35 GHz to 9.0 GHz. Ideal switches will be replaced with real swiches such as pin-diode, which determine that this antenna can work in actual environment. The proposed antenna is suitable to be used in GPS, LTE and wideband wireless communication applications. Acknowledgements The authors would like to acknowledge the Ministry of Education (MoE) Malaysia, Universiti Teknologi Malaysia (UTM) under the research grants (Vote No: 14J18 and 15H97) and Advanced RF and Microwave Research Group (ARFMRG) for supporting this work. References [1] Chin SJ, Abd Aziz MZA, Ahmad MR. Microstrip-Fed Circular Disc Monopole Antenna with Defected Waveguide Structures. International Journal of Electrical and Computer Engineering (IJECE). 2018; 8(1): 189-197. [2] Boutejdar A, Salamin MA, Challal M, Das S, Hani SE, Bennani SS, Sarkar PP. A Compact Wideband Monopole Amtenna using Single Open Loop Resonator for Wireless Communication Applications. TELKOMNIKA Telecommunication Computing Electronics and Control. 2018; 16(5): 2023-2031. [3] Hamdouni AE, Tajmouati A, Zbitou J, Errkik A, Abdellaoui LE, Latrach M. A New Design of an UWB Circular Fractal Printed Antenna. TELKOMNIKA Telecommunication Computing Electronics and Control. 2018; 16(5): 1931-1938.
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