active electronically scanned array
TRANSCRIPT
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ACTIVE ELECTRONICALLY STEERED ARRAY RADAR
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Outline
What is RADAR?
Radar Scanning?
Phased Array Radars
Progress
Future Tasks
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WHAT IS RADAR?RADAR SCANNING?
PHASED ARRAY RADARS
PROGRESS
FUTURE TASKS
Outline
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What is RADAR?
RADAR an acronym for:
Radio Detection and Ranging
Basic Principles Transmits an electromagnetic signal modulated
with particular type of waveform. (modulationdepends on requirements of application)
Signal is reflected from target
Reflected signal is detected by radar receiver andanalyzed to extract desired information
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Basic Operation [5]
Target Range, R=c t / 2
is needed to account for the two-waytime delay
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Frequency Bands [6]
SRE: Surveillance Radar
ASR: Airport surveillance Radar
PAR: Phased array radar
SMR: Surface movementRadar
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Applications (1/2) [1]
Air Traffic Control
Monitor the location of aircraft in flight
Monitor the location of aircraft/vehicles on surfaceof airports
Air Navigation
Weather radar
Terrain avoidance and terrain following
Radar altimeter
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Applications (2/2) [1]
Marine
Law Enforcement and highway safety
Space Military
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Types [5]
Basic Types
Monostatic - transmitter and receiver use same
antennaPulse Transmission
Bistatic - transmitter and receiver antennas areseparated, sometimes by large distances
Continuous wave Transmission
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Generic Radar System [1]
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Generic Radar System [3]
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Functional Descriptions [3]
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WHAT IS RADAR?
RADAR SCANNING?PHASED ARRAY RADARS
PROGRESS
FUTURE TASKS
Outline
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RADAR scanning [4]
An important part of RADAR architecture
Provides support to the antenna
Directs the antenna beam Transmission & Reception
Types:
Surface based scanning
Air borne scanning
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Common elements of Scanners
(1/2) [4] Antenna
Transmit/ Receive RF energy
Single element/ Array Parabolic reflectors, Aperture antennas etc
Transmission Line
Coaxial line or Wave guides
Special rotary joints required to support scanningrotation
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Common elements of Scanners
(2/2) [4] Scan mechanism
Continuous rotation of the antenna about its axis
Usual rate of rotation 4-6 rpm (ground or shipsearch)
Air-borne rotation at 30 rpm
2D rotation- Complex rotation mechanism
Kinematics of the Scan
Data transmission
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WHAT IS RADAR?
RADAR SCANNING?
PHASED ARRAY RADARSPROGRESS
FUTURE TASKS
Outline
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Phased Array Radars (1/2)
No physical rotation of antenna elements for
Scanning
Phase manipulation/ control of the individualantenna
Constructive and Destructive interference
Beam steering in the particular direction
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Phased Array Radars (1/2)
Demonstration [6]Phase control to
steer antenna
beam in the
desired direction
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Beam steering mathematics [6]
Constant phase increment
x = d sin s
360
=
(2
) x
=
360 d sin s
= phase shift between two successive elementsd= distance between the radiating elements (half the wavelength)
s = beam steering
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Example [6]
A radar set works with a wavelength of=3 cm.
The distance between the radiating elements is 1.5 cm.
The beam steering is s= 40.
Which value shallhave to have the phase shifter no. 8?
=(360*1.5 cm/3 cm)*sin(40) = 115.70.
Phase shift value 8 = 7 115.70 = 809.91.
8= 89.91.
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Whats Unique to PAR?
Parabolic Antenna Single radiation element
Single transmitter
Single receiver
Non-conformal
Fixed beam pattern
Mechanical steering
Phased Array Antenna Multiple radiation
elements
Multiple transmitters
Multiple receivers
Conformal
Variable beam pattern
Electronic steering
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Types of Phased Array Radars
[8] Passive phased array radar
Active phased array radar
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System Components
Amplification, Phase shifting and Attenuators
required at each antenna element
High power amplifiers, Low noise amplifier,Limiters
Transmit and Receive circuitry connected to
each antenna element
TR switch, duplexer
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Transmit/ Receive module [6],
[3]
Single Transmit/ Receive element for Active phased arrayradar
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Phase and Amplitude Control
Adding phase shift in the signal
Null and Side lobe control
Anti Jamming
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Transmission Line Phase
shifters [6]
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Digital Beam Steering/ Forming
[8] Use of computational and programmable
environment
Signal processing in the Digital domain
Phase and Amplitude control
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Digital Beam forming [8]
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WHAT IS RADAR?
RADAR SCANNING?PHASED ARRAY RADARS
PROGRESSFUTURE TASKS
Outline
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1.Simulation: Beam Steering
Bram Steering
4 element antenna array
Center frequency: 8 GHz
Phase shifting
Manually for proof of concept
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1. 4-element array at 8GHz
A1 A2 A3 A4
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1.Results (0,0,0,0)
-80
-60
-40
-20
0 20 40 60 80-100
100
-50
-40
-30
-20
-10
-60
0
THETA
Mag.
[dB
]
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1.0,0,0,30
-80
-60
-40
-20
0 20
40
60
80
-100
100
-50
-40
-30
-20
-10
-60
0
THETA
.[B]
m1
m1THETA=
B(Ecross)=-1.135Max
-3.000
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1.0,0,0,45
-80
-60
-40
-20
0 20
40
60
80
-100
100
-50
-40
-30
-20
-10
-60
0
THETA
Mag.
[B]
m1
m1THETA=
B(Ecross)=-1.120Max
-4.000
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1.0,0,0,90
-80
-60
-40
-20
0 20
40
60
80
-100
100
-50
-40
-30
-20
-10
-60
0
E A
ag.
[
]
1
m1E A=
dB(Ecro =-1.101ax
-7.
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1.0,0,0,120
-80
-60
-40
-20
0 20
40
60
80
-100
100
-50
-40
-30
-20
-10
-60
0
E A
ag.
[dB]
m1
m1E A=
dB(Ecro =-1. 77Max
-10.
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1.0,30,90,150
-80
-60
-40
-20
0 20
40
60
80
-100
100
-50
-40
-30
-20
-10
-60
0
THETA
Mag.
[dB]
m1
m1THETA=dB(Ecross)=-1.091Max
-14.000
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1.0,45,90,135
-80
-60
-40
-20
0 20
40
60
80
-100
100
-50
-40
-30
-20
-10
-60
0
THETA
Mag.
[dB]
m1
m1THETA=dB(Ecross)=-1.106Max
-13.000
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1.0,60,120,180
-80
-60
-40
-20
0 20
40
60
80
-100
100
-50
-40
-30
-20
-10
-60
0
T T
Mag.
[d
]
m1
m1T Td ( cross) -1.075Max
-17.000
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1.0,90,180,270
-80
-60
-40
-20
0 20
40
60
80
-100
100
-50
-40
-30
-20
-10
-60
0
THETA
Mag.
[dB]
m1
m1THETA=dB(Ecross)=-0.989Max
-26.000
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2.Simulation: System Architecture
Transmitter module
Baseband signal at 100 MHz
RF converted frequency at 10 GHz
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2.Transmitter model
4
4
4
4
TransmitAntenna
HPAGain 5 dB
Wave form GeneratorBaseband Signal 100 MHz
Upconversion StageLO= . GHzRF=10 GHz
````
1 3
1 3
1 3
1 3
Envelope
Env1
Step=10 nsec
Stop=100 nsec
Order[3]=3Order[2]=3
Order[1]=3Freq[3]=10GHz
Freq[2]=1.0 GHzFreq[1]=100MHz
ENVELOPE
Amplifier2AMP4
S12=0
S22=dbpolar(-40,180)S11=dbpolar(-40,0)
S21=dbpolar(20,0)
Amplifier2AMP3
S12=0S22=dbpolar(-40,180)
S11=dbpolar(-40,0)S21=dbpolar(20,0)
Amplifier2
AMP2
S12=0
S22=dbpolar(-40,180)S11=dbpolar(-40,0)
S21=dbpolar(20,0)
Amplifier2AMP1
S12=0
S22=dbpolar(-40,180)S11=dbpolar(-40,0)
S21=dbpolar(20,0)
BPF_Chebyshev
BPF7
Astop=30 dBBWstop=8 GHz
Ripple=0.1 dBBWpass=50 MHz
Fcenter=10GHz
Amplifier2IF_Amplifier3
S12=0
S22=dbpolar(-40,180)S11=dbpolar(-40,0)
S21=dbpolar(30,0)
MixerWithLO
MIX8
ConvGain=dbpolar(18,0)DesiredIF=RF plus LO
ZRef=50 Ohm
antenna_gain
X4
P_1Tone
Source3
Freq=100MHz
P=polar(dbmtow(0),0)Z=50 Ohm
Num=3
Term
Term5
Z=50 Ohm
Num=5
BPF_ChebyshevBPF6
Astop=30 dBBWstop=8 GHz
Ripple=0.1 dBBWpass=50 MHz
Fcenter=10GHz
Amplifier2IF_Amplifier2
S12=0S22=dbpolar(-40,180)
S11=dbpolar(-40,0)S21=dbpolar(30,0)
MixerWithLOMIX7
ConvGain=dbpolar(18,0)DesiredIF=RF plus LO
ZRef=50 Ohm
antenna_gainX3
P_1ToneSource2
Freq=100MHz
P=polar(dbmtow(0),0)Z=50 Ohm
Num=2
TermTerm4
Z=50 Ohm
Num=4
BPF_Chebyshev
BPF5
Astop=30 dB
BWstop=8 GHzRipple=0.1 dB
BWpass=50 MHz
Fcenter=10GHz
Amplifier2
IF_Amplifier1
S12=0
S22=dbpolar(-40,180)S11=dbpolar(-40,0)
S21=dbpolar(30,0)
MixerWithLO
MIX6
ConvGain=dbpolar(18,0)
DesiredIF=RF plus LO
ZRef=50 Ohm
antenna_gain
X2
P_1Tone
Source1
Freq=100MHzP=polar(dbmtow(0),0)
Z=50 OhmNum=1
TermTerm3
Z=50 OhmNum=3
Term
Term2
Z=50 Ohm
Num=2
P_1Tone
Source
Freq=100MHzP=polar(dbmtow(0),0)
Z=50 Ohm
Num=1
antenna_gain
X1
MixerWithLO
MIX5
ConvGain=dbpolar(18,0)DesiredIF=RF plus LO
ZRef=50 Ohm
Amplifier2IF_Amplifier
S12=0
S22=dbpolar(-40,180)S11=dbpolar(-40,0)
S21=dbpolar(30,0)
BPF_Chebyshev
BPF4
Astop=30 dB
BWstop=8 GHz
Ripple=0.1 dBBWpass=50 MHz
Fcenter=10GHz
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2.Baseband spectrum
0.2 0.4 0.6 0.80.0 1.0
-90
-80
-70
-60
- 0
-40
- 0
-20
-10
-100
0
fr GH
B(v
r("1
"))
2m2
fr =
B(v r("1"))=-9.914time=100.0000nsec
100.0MH
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2.RF level: 10 GHz
6 7 8 9 10 11 12 13 145 15
-70
-40
-10
20
-100
50
fr Hz
dB(
ar("4"))
m3
m3frdB( ar("4")) 33.811tim =100.0000ns c
10.00GHz
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2.Receiver Model
LNA stageecei e Antenna Array
a1
Vout4 a4
Vout3 a3
Vout2 a2
Vout1
VA
VA
1
arget_location=-1A
p_gain=30
EqnVar
antenna_gain
antenna2
antenna_gain
antenna4
antenna_gain
antenna3
antenna_gainantenna1
target_phaseshiftertarget_th1
X=
arget_location
A
plifier2
AMP1
12=0
22=polar(0,180)
11=polar(0,0)
21=dbpolar(A
p_gain,0)
A
plifier2
AMP2
12=0
22=polar(0,180)
11=polar(0,0)
21=dbpolar(A
p_gain,0)
A
plifier2AMP3
12=0
22=polar(0,180)
11=polar(0,0)
21=dbpolar(A
p_gain,0)
A
plifier2
AMP4
12=0
22=polar(0,180)
11=polar(0,0)
21=dbpolar(A
p_gain,0)
er
er
4
=50
h
Nu
=4
er
er
3
=50
h
Nu
=3
er
er
2
=50
h
Nu
=2
er
er
1
=50
h
Nu
=1
PF_ utterworth
PF4
Astop=20 d
Wstop=3
HzApass=3.0103 d
Wpass=25 MHzFcenter=1
Hz
PF_ utterworth PF3
Astop=20 d Wstop=3
Hz
Apass=3.0103 d
Wpass=25 MHzFcenter=1
Hz
PF_ utterworth
PF2
Astop=20 d
Wstop=3
HzApass=3.0103 d
Wpass=25 MHzFcenter=1
Hz
PF_ utterworth PF1
Astop=20 d
Wstop=3
Hz
Apass=3.0103 d
Wpass=25 MHzFcenter=1
Hz
Har
onic alance
H 1
rder[1]=6Freq[1]=1.0
Hz
HA
MONI
ALAN
E
Vt
Vt1
Vt1=vt(vout,0,0,10nsec,201)
t
Vt
Vfc
Vfc1
Vfc1=vfc(vout,0,{1})
f
Vf c
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2.Target Model
v_s
v_s
v_s
v_s
Vf_Pulse
SRC4
Harmonics=16
Weight=no
Delay=0 nsec
Fall=0.1 nsec
Rise=0.1 nsec
Width=0.3 nsec
Freq=1 GHz
Vdc=0 VVpeak=1 uV
Vf_PulseSRC3
Harmonics=16
Weight=no
Delay=0 nsec
Fall=0.1 nsec
Rise=0.1 nsec
Width=0.3 nsec
Freq=1 GHz
Vdc=0 V
Vpeak=1 uV
Vf_Pulse
SRC2
Harmonics=16
Weight=noDelay=0 nsec
Fall=0.1 nsec
Rise=0.1 nsecWidth=0.3 nsec
Freq=1 GHz
Vdc=0 V
Vpeak=1 uV
Vf_PulseSRC1
Harmonics=16
Weight=no
Delay=0 nsec
Fall=0.1 nsec
Rise=0.1 nsec
Width=0.3 nsec
Freq=1 GHzVdc=0 V
Vpeak=1 uV
TimeDelay
TD4
ZRef=50. Ohm
Delay=X*0.108e-9
TimeDelay
TD3
ZRef=50. Ohm
Delay=X*0.081e-9
TimeDelayTD1
ZRef=50. Ohm
Delay=X*0.027e-9
TimeDelayTD2
ZRef=50. Ohm
Delay=X*0.054e-9
Port
P4
Num=4
PortP3
Num=3
Port
P2
Num=2
Port
P1
Num=1
0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.80.0 2.0
-400
-200
0
200
400
-600
600
time, nsec
ts(Vout1),nV
ts(Vout2),nV
ts(Vout3),nV
ts(Vout4),nV
0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.80.0 2.0
0.0
0.2
0.4
0.6
0.8
1.0
-0.2
1.2
time, nsec
ts(v_
s),
V
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2.Target: if Straight
0.2 0.4 0.6 0.8 1.0 1. 2 1.4 1.6 1. 80.0 2.0
-400
-200
0
200
400
-600
600
time, n ec
ts(Vout1,nV
ts(Vout2
,nV
ts(Vout3
,nV
ts(Vout4
,nV
0.6 0.7 0.8 0.9 1.0 1.1 1. 2 1.3 1.40.5 1.5
-130
-120
-110
-100
-90
-140
-80
freq, H
phase(Vout1
phase(Vout2
phase(Vout3
phase(Vout4
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2.In this case, Target Located
10 degrees right
0. 0. 0. 0.
.0 1. 1. 1. 1.
0.0 2.0
-400
-200
0
200
400
-600
600
t me, se
t
s(V
t1),
V
t
s(V
t2),
V
t
s(V
t
),
V
t
s(V
t4),
V
0.6 0.7 0.
0.!
1.0 1.1 1.2 1."
1.40.5 1.5
-130
-120
-110
-100
-90
-140
-80
freq, GHz
phase(V
#
$
t1)
phase(V
#
$
t2)
phase(V
#
$
t3)
phase(V
#
$
t4)
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2.Target Located 10 degrees
left
0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.80.0 2.0
-600
-400
-200
0
200
400
600
-800
800
t% &
'
,ns'
c
ts(V
t1),nV
ts(V
t2),nV
ts(V
t3),nV
ts(V
t4),nV
0.6 0.(
0.8 0. ) 1.0 1.1 1.2 1.3 1.40.0
1.0
-0
0
-40
-30
-20
-10
0
10
20
30
40
0
0
-60
60
fr , z
s
(V
t1)
s
(V
t2)
s
(V
t3)
s
(V
t4)
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WHAT IS RADAR?
RADAR SCANNING?PHASED ARRAY RADARS
PROGRESS
FUTURE TASKS
Outline
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Future Tasks
1. System Level simulation
Beam Steering
Complete architecture
2. Component Design
a. Muhammad Usman Afzal
High power Amplifier
Antenna Array
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References
1. ELEC4600 Radar and Navigation
Engineering
2. Radar Principles & Systems byLT Mazat3. Introduction to Radar Systems, MIT Lincoln
Laboratory
4. Radar Scanners & Radomes, MIT radiation
laboratory series
5. Introduction to Radar basics Matlab
simulation for Radar system design
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References
6. www.radartutorial.eu
7. Active Phased Array Radar Systems, Dr.
Yasser Al-Rashid. Lockheed Martin MS2Radar Systems
8. Phased Array Antenna And Beam Forming
Sub-sytems In Phased Array Radar
Dr A. Jhansi Rani, A.Jaya Lakshmi,International Journal of Engineering Science
and Technology