Fundamentals of Antennas Carlos A. Fernandes
Transcript of Fundamentals of Antennas Carlos A. Fernandes
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Antennas and Propagation - Master in Aerospace Engineering
Carlos A. Fernandes
Fundamentals of Antennas
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ANTENNAS AND PROPAGATION - MAero [email protected] 2
Source Transmission structure Antenna Radiation
4.1 Introduction to antennas
๐๐๐๐ป๐ฌ
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Source Transmission structure Antenna Radiation
4.1 Introduction to antennas
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4.1 Introduction to antennas
Most visible type of antennas
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Half-wavelength dipole radiation
l / 2
4.4 Antenna radiation
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Can be viewed as a section of a largerantenna
jyx
z
r
Rq
iq
ijir
dldl < l
4.2 Hertz dipole
เดฅ๐ =๐
4๐าง๐ ๐๐
๐โ๐๐ ๐
๐
Infinitesimal current
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Radiation fields
4.2 Hertz dipole
2๐ ฮค๐ ๐ sphericalwave
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Radiation fields
4.2 Hertz dipole
jy
x
z
r
Rq
iq
ijir
dl
Infinitesimal current
sphericalwave
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4.3 Radiation pattern
= โ ๐บ + ๐ โ ๐บ (๐๐๐๐๐๐๐ ๐๐๐ ๐)
๐ = ๐2 ๐บ
z
x
y
j
3๐ท ๐๐๐๐๐๐ ๐๐๐ก๐๐ก๐๐๐ ๐๐ ๐/๐๐๐๐ฅโ (sin ๐)๐
(๐๐๐๐๐๐๐๐๐๐๐ก ๐๐ ๐ ๐๐๐ ๐ป. ๐ท. )
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Polar representation
4.3 Radiation pattern
๐ธ โ ๐๐๐๐๐ ๐ป โ ๐๐๐๐๐
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Polar representation
4.3 Radiation pattern
๐ธ โ ๐๐๐๐๐ ๐ป โ ๐๐๐๐๐
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50 40 30 20 10 0
(u1)
(u2) (u3)AL360P AL560
AL760
Anechoic chamber โ roll over azimuth configuration
(g2) (g3)
(g1)
RXTX
Controller
PC
4.3 Radiation pattern
Antena under test
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Receive antenna
Antenna under test
Main lobe
Secondary lobes
4.3 Radiation pattern
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Anechoic chamber โ roll over azimuth configuration
4.6 Radiation pattern
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4.3 Radiation pattern
Types of radiation pattern
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Rectangular horn (directive pattern)
4.3 Radiation pattern
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4.4 Directivity and Gain
~๐๐
๐๐
Geometry
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4.4 Directivity and Gain
Directivity of Hertz dipole
,
เถฑsin3๐ = โ3
4cos( ๐) +
1
12cos(3๐)
๐(๐)
โ ๐ท = 1.5 @ ๐ =๐
2(1.76 dBi)
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4.4 Directivity and Gain
Directivity estimation๐1
๐๐ โ ๐๐เถฑ
0
2๐
เถฑ
0
๐1
sin ๐ ๐๐ ๐๐ = 2๐๐๐ โcos๐ 0๐1
= 2๐๐๐ โcos๐1 + 1 ๐๐ ๐ โช 1, cos๐ โ 1 โ๐2
2
= ๐ ๐๐ ๐12 =
๐
4๐๐ ๐3๐๐ต
2 โ ๐๐ ๐3๐๐ต2
(๐๐๐ฅ๐๐๐ข๐ ๐๐๐๐๐๐ก๐๐ฃ๐๐ก๐ฆ)
๐ท =4๐ ๐๐
๐๐ ๐3๐๐ต2
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4.4 Directivity and Gain๐ท(๐, ๐) =
๐(๐, ๐)
๐๐/4๐
~๐๐
๐๐
Gain
๐บ(๐, ๐) =๐(๐, ๐)
๐๐/4๐
[dBi]
๐บ๐๐ต = 10 log๐บ
๐บ๐๐๐[dBd]
ฮคฮป 2 dipole
๐บ๐๐๐ = 1.64
ฮi = 0=๐๐๐๐
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1 medida
2 medida
~
AETSonda
PP
Sonda
P~P
Cornetapadrao
G [dBi]
f [GHz]
Aspecto tipico da curva de calibracao
de uma corneta padrao
Gain comparison method
๐บ๐๐ต = ๐บ๐๐๐ต + ๐1๐๐ต๐ โ ๐2๐๐ต๐
๐บ
๐บ๐
4.4 Directivity and Gain
๐๐ ๐1
๐2๐๐
1๐ ๐ก ๐๐๐๐ ๐ข๐๐๐๐๐๐ก
2๐๐ ๐๐๐๐ ๐ข๐๐๐๐๐๐ก
๐ด๐๐๐๐๐๐๐
๐๐๐๐๐๐๐ก๐ ๐๐๐๐โ๐๐๐
๐1 โ ๐บ ๐๐
๐2 โ ๐บ๐ ๐๐
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4.5 Input impedance
๐๐ด = ๐ ๐ + ๐ ๐ฟ + ๐ ๐๐ด
~๐ ๐ด
๐๐ด
๐๐
Application to the Hertz dipole
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Hertz dipole l/2 dipole
4.5 Input impedance
๐๐ด = ๐ ๐ + ๐ ๐ฟ + ๐ ๐๐ด = ๐ ๐ด + ๐ ๐๐ด
= 0 in the resonance
๐น๐๐๐ [GHz] ๐น๐๐๐ [GHz]
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4.5 Input impedance (l/2 dipole)
|๐ค|
1.5 GHz
2.2 GHz
๐ฉ~๐๐%
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Polarization elipse
4.6 Polarization
iq
ij
โฐ(t)
b
a g
Eq
Ejleft-hand
right-hand
linear,
circular
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Polarization mismatch (coordinate system)
4.6 Polarization
๐๐ = เดค๐i โ เดค๐aโ 2 = cos าง๐
2ฦธ๐ข๐
ฦธ๐ข๐
เท๐a
เท๐i๐
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q
180 90 0 90 180
180 90 0 90 180
4.7 Phase center
d
Eixo de rotaรงรฃo
Posiรงรฃo do centro de fase
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4.8 Band width
Gain, SLL
Input impedance
Polarization
Efficiency
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Input reflection of l/2 dipole vs frequency
4.8 Band width
Reflection coefficient โ magnitude and phase
๐ฟ๐ต =0.15 GHz
1.8 GHz= 8.33%
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Input reflection of a UWB antenna
4.8 Band width
Reflection coefficient โ magnitude
๐ฟ๐ต 3.5 โถ 1
10.5 ๐บ๐ป๐ง
3 GHz
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Received power, Friis formula
4.8 Effective aperture
๐๐ ๐ด
[W/m2] [m2]
๐๐
๐๐ฟAntenna
Load
๐๐ =1
2๐ ๐ฟ ๐ผ๐ฟ
2 =๐๐ฟ
2๐ ๐ฟ2 ๐๐ด + ๐๐ฟ
2=
๐๐ฟ2
8 ๐ ๐๐๐๐ ๐๐ฟ = ๐๐ด
โ
๐๐ =
เดฅ๐ฌ ๐
2 ๐0
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Received power, Friis formula
4.8 Effective aperture
๐๐ฟAntenna
Load๐๐ = ๐๐๐ด๐๐ ๐๐ =
๐๐ฟ2
8 ๐ ๐๐ด๐๐ =
1
๐๐
๐๐ฟ2
8 ๐ ๐
Application to the Hertz dipole
๐โ โช โ
๐ = เดค๐ธ ๐โ
=เดฅ๐ฌ 2
2 ๐0๐ด๐๐ =
3๐2
8 ๐
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Received power, Friis formula
4.8 Effective aperture
๐๐ฟAntenna
Load
๐โ โช โ
๐ด๐๐ =3๐2
8 ๐
๐ท = ๐๐ ๐ด๐๐
3
2= ๐๐
3๐2
8 ๐๐๐ =
4๐
๐2๐ท =
4๐
๐2๐ด๐๐
๐2๐1 =๐2
๐ด๐๐
Universal constant
Use Hertz dipole results to obtain ๐๐
๐ท = 1.5
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Received power, Friis formula
4.8 Effective aperture
๐บ๐(๐๐, ๐๐)
๐ ๐บ๐ (๐๐ , ๐๐ )
ReceiverMatchingcircuit
Matchingcircuit
Free space loss
๐๐ ๐ =๐๐
4๐๐2[๐/๐2]๐บ๐ ๐๐ , ๐๐
๐๐ ๐ =๐๐
4๐๐2[๐]๐บ๐ ๐๐, ๐๐ ๐ด๐๐ (๐๐ , ๐๐ )
๐๐ (๐) = ๐๐ ๐บ๐ ๐๐ , ๐๐ ๐บ๐ ๐๐ , ๐๐
๐
4 ๐ ๐
2
[๐]๐๐ ๐๐ ๐๐
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Received power, Friis formula
4.8 Effective aperture
๐
๐บ๐(๐๐, ๐๐)๐บ๐ (๐๐ , ๐๐ )
ReceiverMatchingcircuit
Matchingcircuit
๐๐ = ๐๐ ๐บ๐ ๐๐ , ๐๐ ๐บ๐ ๐๐ , ๐๐
๐
4 ๐ ๐
2
๐๐ ๐๐ ๐๐
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What is the limit on the received power (ex communications)
๐๐ = 43 ๐๐ต๐, ๐บ๐ = 20 ๐๐ต๐, ๐บ๐ = 73 ๐๐ต๐, ๐ = 280 Mkm, ๐ = 8 GHz
๐๐ = โ143. 5 ๐๐ต๐ (down-link usually not done directly )
4.9 Thermal noise
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4.9 Thermal noiseEffect on received power (ex radiation pattern measurement)
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Noise in a resistor
Electrons in any resistor ๐ at physical temperature ๐ โ 0 exhibit random
motion, responsible for a fluctuating resistance, and associated fluctuating
voltage across the resistor terminals ๐ = 0, ๐๐๐๐ = ๐2 โ 0. It exists
even if a current is not flowing in the resistor.
๐
๐
Physical resistor in open circuit
๐๐๐๐
๐พ Boltzman constant, 1.38 ร 10โ23 [J/K]
๐ Absolute physical temperature [K]
โ๐ Bandwidth [Hz]
Ex: ๐ = 300 ๐พ, ๐ = 50 ๐บ, โ๐ = 10 ๐๐ป๐ง โ ๐๐๐๐ = 2.88 ๐๐
๐๐๐๐ = 4 ๐พ ๐ ๐ โ๐ [V]
Nyquist and Johnson (researchers from Bell
Labs) showed in 1928 that, in open circuit,
the root mean square of this voltage is
4.9 Thermal noise
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the noise power transferred to the load is
4.9 Thermal noiseNoise in a resistor
๐ =๐๐๐๐ 2
4 ๐
๐
๐ ๐
Equivalent circuit
๐
๐
Physical resistor
โIdeal noiselessโ
resistors
Resistor ๐ connected to a load with the same value ๐
The transferred noise power is independent of ๐ value (as long
as the load has the same value as the resistor).
๐๐๐๐
๐๐๐๐
Ex: ๐ = 300 ๐พ, โ๐ = 10 ๐๐ป๐ง โ ๐ = 0.0414 ๐๐ (โ103 ๐๐ต๐)
๐๐๐๐ = 4 ๐พ ๐ ๐ โ๐
๐ = 150 ๐พ โ ๐ = 0.0414 ๐๐ (โ106 ๐๐ต๐)
= ๐พ ๐ โ๐
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4.9 Thermal noiseEquivalent noise temperature
Very small noise power values are impractical to handle in calculations. It is easier to introduce the concept of equivalent noise temperature ๐๐ even if the loss mechanism is not purely thermal, and work only with these temperatures instead.
๐๐ =๐
๐พ โ๐
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4.10 Antenna noise temperatureInternal noise temperature
Antennas contribute with two noise terms:
๐๐ด๐ associated with its loss resistance ๐ ๐ฟ๐๐ด๐ associated with external noise captured through the radiation
pattern.
๐๐ = ๐ ๐๐๐ =๐ ๐๐๐
๐ ๐๐๐ + ๐ ๐ฟ๐๐๐
๐๐ด๐ = ๐พ ๐๐ด 1 โ ๐ ๐ฅ๐
๐๐๐ = ๐๐ ๐ด๐๐ ๐๐
๐๐ด = ๐๐ด๐ + ๐๐ด๐
๐๐ด๐ = ๐๐ด 1 โ ๐
๐พ ๐ฅ๐ ๐๐ด = ๐พ ๐ฅ๐( ๐๐ด๐ + ๐๐ด๐) ๐๐ด = ๐๐ด๐ + ๐๐ด๐
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4.10 Antenna noise temperatureExternal noise temperature
๐๐ด๐ =1
4๐เถฑ
0
2๐
เถฑ
0
๐
๐๐ต ๐, ๐ ๐บ ๐, ๐ sin ๐ ๐๐ ๐๐
๐บ ๐, ๐ - Antenna radiation pattern
External noise sources associated with ๐๐ด๐:
โข Man-made noise;
โข Atmospheric noise;
โข Galactic noise;
โข Cosmic background.
๐๐ด๐ = ๐พ ๐๐ด๐ โ๐
๐๐ต ๐, ๐ = ๐ ๐๐ is the brightness temperature of the source, where ๐๐is the physical temperature of the source and its emissivity is 0 < ๐ < 1
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A โ Quiet Sun
B โ Moon
C โ Galactic noise
D โ Cosmic background
4.14 Noise temperatureBrightness temperature
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Antenna noise temperatureExternal noise temperature
๐๐ด๐ โ ๐๐ต ๐0, ๐01
4๐เถฑ
0
2๐
เถฑ
0
๐
๐บ ๐, ๐ sin ๐ ๐๐ ๐๐
External noise sources associated with ๐๐ด๐:
In the specific case of a high directivity antenna, when its beamwidthcaptures only a small portion of an extended noise source, so that ๐๐ต ๐, ๐ can be considered constant within the antenna main beam, we can write:
= 1๐๐ด๐ โ ๐๐ต ๐0, ๐0
Extendednoise source