Antennas and Fundamental Parameters February 20, 2019...Definition of Antenna The guiding device or...
Transcript of Antennas and Fundamental Parameters February 20, 2019...Definition of Antenna The guiding device or...
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Fundamental Parameters and
Figures-of-Merit of Antennas
Constantine A. Balanis
Arizona State University
Tempe, AZ 85287 5
balanis@asu.
706
edu
Copyright©2016 by Constantine A. Balanis All rights reserved IEEE EMC, Phoenix, AZ, Section
March 20, 2019
Copyright©2016 by Constantine A. Balanis All rights reserved IEEE EMC, Phoenix, AZ, Section
March 20, 2019
AntennasSingle Elements and Arrays
'Electronic Eyes and Ears of the Worl
J
Antenn
ohn D.
d'
K
as:
raus
Antenna As A Transition/Transducer Device
Antenna
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TE Horn Animation
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TM Open Animation
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TM Box Animation
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2
Copyright©2016 by Constantine A. Balanis All rights reserved IEEE EMC, Phoenix, AZ, Section
March 20, 2019
Definition of AntennaAccording to the
:
"A means for radiating or receiving
According to t
rad
he :
"A means for radiating or receiving radio waves
io waves "
.
.
Webs
IE
ter'
EE S
s Dictio
tandard Definitions
of Terms for Antennas
nary
In other words, the antenna is the
between free-space and
a guiding device.
"
transitional
structure / transducer
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March 20, 2019
Definition of Antenna
The guiding device or transmission line
may take the form of a coaxial line or a
hollow pipe (waveguide), and it is used
to transport EM energy from the transmitting
source to the antenna, or from the
In the former case, we have a
antenna and in the latter a antenna.
antenna
to the recei .
ver
transmitting
receiving
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Definition of Antenna
In addition to receiving or transmitting EM energy,
an antenna in an advanced wireless communications
the radiation energy in some direction
system is usually required
s and
to optimize or accentuate
s
Thus the antenna must also serve as
directional devi
a
, in addition
it in
to a
.
rce adiating device
othe
.
rs
uppress
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Thevenin EquivalentIn Transmission Mode
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Horn Antenna And Its Equivalent
RL
Horn Equivalent
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Types of Antennas
1. Wire antennas2. Aperture antennas3. Microstrip antennas4. Array antennas5. Reflector antennas6. Lens antennas7. Other Antennas for Mobile Units
3
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Fundamental
Parameters
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Coordinate Systemfor
Antennas
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Coordinate System
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Coordinate System
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2 22
0 0 0 0
22
0 0
!
Area of Sphere s
Spherical Angular Limits
in
Area sin
Area 2 1 1 0 ! !
dA r d d
r d d
0
20
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2 22
0 0 0 0
22
0 0
2 2
Area of Sphere s
Spherical Angular Limits
in
Area sin
Area 2 2 4
dA r d d
r d d
r r
20
0
4
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ˆ ( , )a E H
ˆ ( , )a E H
ˆ ( , )r r ra E H
Spherical Electric and Magnetic Field Components
spherical
right hand
coordinate syst
ˆ
e
ˆˆ
ˆ
m
ˆ r
a
aa
aa
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• Field Pattern:
A plot of the field (either electric |E| or magnetic |H|) on a linear scale
• Power Pattern:
A plot of the power (proportional to either the electric |E|2 or magnetic |H|2
fields) on a linear or decibel (dB) scale.
Amplitude Radiation Pattern
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March 20, 2019
Linear ScaleN = 10 elementsd = /4 spacingHPBW = 38.64o
2-D Normalized Field |En| Pattern of a Linear Array
0.707 0.707
HPBW
|Er|
+ +
++
+ +-
--
--
Field Pattern(linear scale)
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
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March 20, 2019
2-D Normalized Power |En|2 Pattern
of a Linear Array
Linear ScaleN = 10 elementsd = /4 spacing
HPBW = 38.64o0.5 0.5
HPBW
+ +
-
--
Power Pattern(linear scale)
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
|Er|2
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dB ScaleN = 10 elementd = /4 spacing
HPBW = 38.64o
2-D Normalized Power |En| Pattern of a Linear Array in dB
-3 dB -3 dBHPBW
+ +
++
+ +
-
--
--
Power Pattern(dB)
-35
-30
-25
-20
-15
-10
-5
0
|Er|
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Polar Pattern
x
z
y
Normalized FieldPattern (linear scale)
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
First null beamwidth (FNBW)
Half-power beamwidth (HPBW)
Minor lobes
Major lobe
Side lobe
Minor lobes Back lobe
++
-
+-
-
+-
+ +-
5
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Normalized FieldPattern (linear scale)
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
x
y
z
θ
ˆrE
E
E
Normalized 3-D Amplitude Field Pattern
of Linear Array
Linear Scale N = 10, d
2 2 2
ˆ( , , ) | ( , , )
ˆ + ( , , )
ˆ + ( , , )
| | | | | | | |
cr r r r c
c
c
r
E r a E r
a E r
a E r
E E E E
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Polar (dB Scale): Two-Dimensional Pattern
- -
- -
+ +
Normalized FieldPattern (dB)
-35
-30
-25
-20
-15
-10
-5
0
(l=1.25)
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Directivity D
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0 rad
max max
radmax
10
10
0
0 0
, 4 ,
4
10log(dB) (dimensionless)
(dB) (dimensionles
[ ]
10 log s[ ])
o
D
D D
D
U U
U P
U U
U
D
D D
P
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0
max
0
rad
directivity (dimensionless)
maximum directivity (dimensionless)
radiation intensity (W/unit solid angle)
maximum radiation intensity
radiation intensity of isotropic
radiated power (W)
D
D
U
U
U
P
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DirectivityRealized
Gain
inP
Gain
radP
+inP
+inP
inP
6
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Three-dimensional Directivity Pattern
Directivity(dimensionless)
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
z
yx
D=1
D=1.67sin3( )
1.0
1.67
122.56°
1.67
57.44°
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Two-Dimensional Directivity Pattern
D (dipole)=1.67sin3( )
D (isotropic)=1
57.44°
122.56°
57.44°
122.56°
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rad 0 2
2rad 0
2rad 0
max 0x
0max
2
0 2rad
0
0ma
0
0
E
d
4 141.27 dimensionles
n
s
sin 1 n
x
.2
sin
B
ˆ
sin
s
ample 1:
Solutio
0
in
:
1. 38
7si
rW a Ar
P
AUD
P A
D
U
D
W
D
A
U r A
U A A
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2
rad 0 2
ra
2
max 00
r
d 0
2 2rad 0
m
0
a
d
x 0
a
2
m x
0
0a 2
2
E
sinˆ
8
3
sin
sin
d
xample 2:
Solution:
1.761 dB
l4 4
1.5 imension ess8 3
sin 1.5sin
rW a Ar
P
A
U AD
P
D
A
U r W A
U U A
D
D
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Three-Dimensional Normalized Radiation Patterns
0
2 20
0
0
1.27 1.038 dB
1.5 1
sin
sin 1.5sin
.761 d
1.
B
27sin
D
D D
D
D
D
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7
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0
0
2 2
o o
o o
0
0
12 11 1 2
0
1
1
0
0
1.5sin 1.5sin 1
1sin sin (0.667)
1
(isotropic) : 51.94 128.06
(i
1.27sin 1
1sin 0.
sotropic) : 54.
7871.27
s
.5
sin (0.8165) 54.7
74 125.26
in (0.787) 51
4
.94
D D
D D
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Approximate Formulasfor
Directivity
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Kraus Formula
01 2 1 2
2
01 2 1 2
2
1 2
0 0
1 2
4 4 41, 253
4 1804 41, 253
, sin
A r r d d
r r d d d d
A n r r
D
D
F d d
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0 1 2
0 2 2 2 21 2 1 2
0 2 21 2
1 1 1 1
2
32ln 24 22.18
Arithmetic mea
1
72,
n
815A r r r r
d d
D D D
D
D
Tai & Pereira Formula
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Normalized FieldPattern (linear scale)
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
x
y
z
θ
ˆrE
E
EN = 10 elementsd = /4 spacingHPBW = 38.64o
FNBW = 73.8o
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IEEE EMC, Phoenix, AZ, Section March 20, 2019
01 2 1
0 2 2 21 2
2
0
0 21 2
72,8
Kraus:
Tai & Pereir
4 4 41, 253
41, 253 41, 25327.63 14.51 dB
(38.64)
Di
15 72,81524.38 13.87 dB
2(3
rectivi
10.1158 10.
a:
Using the computer program t ,
05
y
8.64)d d
A r r d d
d d
D
D
D
D
dB
8
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Directional Patterns
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0 20 2
Elsewhere
1,2,3 10,15, 20
cos ,
0
noB
U
n
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Radiation Intensity Pattern
4
(
0 90
, ) co
3
s
0 60
o
o
U
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Exact & Approximate DirectivitiesTable 2.1
5.5n
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Kraus’ Error = 0n = 5.497 5.5
HPBW = 56.35º
|Kraus’ Error|=|T & P’ Error|=6.24% n = 11.28
HPBW = 39.77º
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OmindirectionalPatterns
9
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Omnidirectional Pattern With Minor Lobes Normalized Field
Pattern (linear scale)
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
x y
z
)0
sin0
(2
nU
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Omnidirectional Pattern Without Minor Lobes
Normalized FieldPattern (linear scale)
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
xy
z
)0
sin0
(2
nU
IEEE EMC, Phoenix, AZ, Section March 20, 2019
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IEEE EMC, Phoenix, AZ, Section March 20, 2019
Omnidirectional Patterns
sin ( )0
0 2nU
Directivity:
0 2
0
101
HPBW(degrees) 0.0027[HPBW(degrees)]
1172.4 191 0.818
HPBW(degrees)
D
D
McDonald
Pozar
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March 20, 2019
Gain
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March 20, 2019
DirectivityRealized
Gain
inP
Gain
radP
+inP
+inP
inPCopyright©2016 by Constantine A. Balanis All rights reserved
IEEE EMC, Phoenix, AZ, Section March 20, 2019
Radiation efficiency
Conduction efficiency
Dielectric efficiency
cd c d
c
d
e e e
e
e
(2-49a)00 cdG e D
10
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Antenna Radiation Efficiency
cde
Horn Antenna And Its Circuit Equivalent
RL
Horn Equivalent
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Copyright©2016 by Constantine A. Balanis All rights reserved
Power Radiated by Antenna ( )
Power Delivered
Radiati
to Ant
on Effi
enna
c ency
( )
icd
cd
r
r
d
L
cr
r
L
P
e
e
Re
R R
P P
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IEEE EMC, Phoenix, AZ, Section March 20, 2019
10
1
0
0
10
0
10log
10log ( )
(dB)
(
+10l )
d )
(
B
og
cd
cd
o
o
e
e
DG
G
D
0 0
cd
cd
G
D
e
eG
D
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Antenna Reference Terminals
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RealizedGain
11
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DirectivityRealized
Gain
inP
Gain
radP
+inP
+inP
inPCopyright©2016 by Constantine A. Balanis All rights reserved
IEEE EMC, Phoenix, AZ, Section March 20, 2019
2
2
(1 | | )
antenna total efficiency
(1 | | ) Reflection efficie
Radiation efficiency
Conduction
ncy
( , ) ( , )
( ,
( , )
efficiency
Dielectric effic
( ), ) cd
cd c d
r
d
ore r cd
in
o
e
r in
r e
e
e eD
e
G
G
e
e
D
e
e
D
e
e
iency
Realized Gain Gre
Today antenna technology is
ScienceNotArt
Very bright future and many challenges ahead. We just need exercise creativity,
imagination and science for its advancement.
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March 20 2019