yacouba coulibaly, halim boutayeb and tayeb a. denidni
DESCRIPTION
Gain Enhancement of a Dielectric Resonator Antenna Using a Cylindrical Electromagnetic Crystal Substrate. Yacouba Coulibaly, Halim Boutayeb and Tayeb A. Denidni. Outline. Introduction Antenna Configuration Simulation Results Measurements Conclusion. Introduction. - PowerPoint PPT PresentationTRANSCRIPT
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Gain Enhancement of a Dielectric Resonator Antenna Using a Cylindrical
Electromagnetic Crystal Substrate
Yacouba Coulibaly, Yacouba Coulibaly, Halim Boutayeb and and Tayeb A. DenidniTayeb A. Denidni
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
• Introduction• Antenna Configuration• Simulation Results• Measurements• Conclusion
Outline
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Inconvenient of a Dielectric Resonator Antenna:
low gain
Introduction
Advantages of a Dielectric Resonator Antenna (DRA)
Low losses
Reduced sized
High radiation efficiency
High density integration
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Introduction (cont.)
To improve the radiations characteristics of the DRA, few studies have been proposed:
The DRA has been placed on different ground planes shapes
Coaxially corrugated.
Strip corrugated.
Mushroom-like Electromagnetic Bang Gap (EBG) substrate.
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Introduction (cont.)
Design Objectives
Use a circularly periodic EBG to increase the gain of a cylindrical DRA.
Exciting the fundamental mode
Have the same radiation pattern shapes with or without the EBG substrate
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Antenna Design
Description:A Dielectric Resonator (DR) :
The DRA has a radius R=15mm, a height hd=10.5mm,and a
permittivity εdra=31.5. .
A Coaxial feed line:
The coaxial line is at a distance of 9
mm from the center.A circular EBG :
Printed on a substrate of permittivity ε2=2.2 and thickness
h=3.2mm. The distance from one strip to the following one is g=2mm. The periods for the strips is Pr2=24.6mm.
The metallic via have a radius a=2mm, and they are disposed with the same transversal period and the same radial period Pr2=23.6mm .
To p V ie w
S id e V ie w
x
y
z
x
S u b s tr a teG r o u n d p lan e
Via
g
P r1
P r1
P r1
P r2
P r2
P r2
Viad iam eter = a
D R A
E x c ita t io n( C o ax ia l lin e)
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Simulated return loss Simulated return loss (with Ansoft HFSS)(with Ansoft HFSS) of the antenna with of the antenna with and without the EBG substrateand without the EBG substrate
Simulated results
2,1 2,4-40
-35
-30
-25
-20
-15
-10
-5
0
With EBG Without EBG
S11
(d
B)
Freq (GHz)
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Simulated gain (with Ansoft HFSS) of the antenna with and Simulated gain (with Ansoft HFSS) of the antenna with and without the EBG substratewithout the EBG substrate
Results:
•The gain is increased by 3 dB due:
• to the reduction of the surface waves.• to the coupling between the DRA and the circular EBG (mainly).
Simulated results (cont)
2,10 2,15 2,20 2,25 2,30 2,35 2,405
6
7
8
9
10 With EBG Without EBG
Ga
in (
dB
)
Freq (GHz)
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Simulated radiation patterns at 2.25 GHz, in both the E- and Simulated radiation patterns at 2.25 GHz, in both the E- and H-Plane, with and without the EBG substrateH-Plane, with and without the EBG substrate
Results:
•The EBG structure improves the gain
•The back radiation decrease
Simulated results (cont)
-10
-5
0
5
100
30
60
90
120
150
180
210
240
270
300
330
-10
-5
0
5
10
E- plane H- plane
2.25GHz
Without EBG With EBG
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Experimental results
Photographs of the fabricated antenna prototypesPhotographs of the fabricated antenna prototypes
DRA aloneDRA alone DRA with cylindrical DRA with cylindrical EBG substrateEBG substrate
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Experimental results
2,10 2,15 2,20 2,25 2,30 2,35 2,40-30
-20
-10
0
S11
(dB
)
Frequency (GHz)
Without EBG With EBG
Measured return loss of the antenna with and without the Measured return loss of the antenna with and without the EBG substrateEBG substrate
Network AnalyzerNetwork Analyzer
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
Experimental results (cont)
Measured gain (in an anechoic chamber at INRS) with and Measured gain (in an anechoic chamber at INRS) with and without the EBG substratewithout the EBG substrate
2,10 2,15 2,20 2,25 2,30 2,35 2,404,0
4,5
5,0
5,5
6,0
6,5
7,0
7,5
8,0
8,5
9,0
Ga
in(d
B)
Frequency(GHz)
With EBG Witout EBG
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
H-planeH-planeE-planeE-plane
Measured radiation patterns with and without the EBG Measured radiation patterns with and without the EBG substratesubstrate
-10
0
100
30
60
90
120
150
180
210
240
270
300
330
-10
0
10
W ith EBG Without EBG
-10
0
100
30
60
90
120
150
180
210
240
270
300
330
-10
0
10
W ith EBG Without EBG
Experimental results (cont)
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INRS- Énergie Matériaux Télécommunications Montréal, Québec, Canada
The gain enhancement of a DRA has been investigated and good performances have been achieved
By adding the EBG substrate, the radiation characteristics have been significantly improved
The coupling between the cylindrical DRA and the reduction of the surfaces waves enhance the gain of the antenna
Conclusion
Perspectives:
• Investigation of elliptical EBG structures;• Design of elliptical patch antennas and elliptical DRAs integrated on elliptical EBG substrates, for Satellites communications applications (circular polarization).