1 IDGA Sensors Nov 06 (1) Unclassified 11 OCT 07 . Wittstruck (1) October 11, 2007 U.S. Army . Program Executive Office, Intelligence, Electronic Warfare & Sensors Unclassified Army’s Digital Array Radars Dr. Rich Wittstruck [email protected]
1IDGA Sensors Nov 06 (1) Unclassified11 OCT 07 . Wittstruck (1)
October 11, 2007
U.S. Army . Program Executive Office, Intelligence, Electronic Warfare & Sensors
Unclassified
Army’s Digital Array Radars
Dr. Rich [email protected]
2IDGA Sensors Nov 06 (2) Unclassified11 OCT 07 . Wittstruck (2)
Today’s Counterfire Radar Capabilities
AN/TPQ-48(V)2
• SOF system derivative fielded on operational needs statement
• Only mortars: 1-6.5km• 360° coverage • Range and accuracy
improvements in V3
• Mortars: 0.75-18km• Medium Cannon: 3-14.5km • Rockets: 8-24km• 90° Coverage• Improved Processor On-going
• Medium Cannon: 3-30km • Rockets: 3-50km• 90o Coverage• RMI Initiative• Long Range software initiative in
SWBII+ adds 120KM mode
AN/TPQ-36(8) AN/TPQ-37(8)
50 km
Rocket
Cannon
30 km
Mortar
6.5 kmCannon
Mortar
Rocket
14.5 km
18 km
24 km
3IDGA Sensors Nov 06 (3) Unclassified11 OCT 07 . Wittstruck (3)
GIRAFFE
BACKGROUND
• Air defense radar with an added Counterfire mode
• Countefire performance acceptable for limited target sets
4IDGA Sensors Nov 06 (4) Unclassified11 OCT 07 . Wittstruck (4)
• 128 circuit cards (86 unique)• 20 cubic feet• 3 KW of power• Complex “wired” backplane• Non-programmable• No growth
TPQ-37
• New modern architecture• 100% COTS technology• Non-proprietary• Open architecture• Supports future software requirements• Leverages MPQ-64 software• 3 VME cards• Lighter weight• 0.2 KW of power• Commonality with AN/TPQ-36(V)8
Radar Processor
TPQ-36/37Upgrade
CommonProcessor
Radar Processor Replacement
5IDGA Sensors Nov 06 (5) Unclassified11 OCT 07 . Wittstruck (5)
Transmitter/Cooler
Transmitter Upgrade
6IDGA Sensors Nov 06 (6) Unclassified11 OCT 07 . Wittstruck (6)
Radar LRUs
7IDGA Sensors Nov 06 (7) Unclassified11 OCT 07 . Wittstruck (7)
EQ - 36
• Solid State Antenna
• Remote Operations
• Prognostics Maintenance
• Crew size 4
• Single C-130 lift
• Single vehicle
• Improved Clutter Mitigation
• Warn
• 90º Range
• Mortars – 0.5 to 20 km
• Artillery – 3 to 32 km
• Rockets – 15 to 60 km
• 360º Range (Mortars)
•Light - 3 to 10 km
Medium – 3 to 12
km Heavy – 3 to
15 km
15 Km
3Km
Mortar Cannon
OR
60Km
32Km
20Km
Rocket
Q37 Capabilities
Q36 Footprint
Cannon
Mortar
8IDGA Sensors Nov 06 (8) Unclassified11 OCT 07 . Wittstruck (8)
General Considerations
• Use of spectrum
• Size/Weight/Power– Q37+ performance in Q36 footprint (90 Degree)– Add 360 degree capability
• “-ilities”, especially:– Mobility/Transportability– Survivability– Reliability/maintainability
9IDGA Sensors Nov 06 (9) Unclassified11 OCT 07 . Wittstruck (9)
Endstate
E Q36 Increment I/II
ATNAVICS
Sentinel
• 90° Coverage• 60Km for Artillery• 300Km Max Range for Missiles• Single Sortie C-130
Long Range Counterfire Radar
• Counterfire Target Acquisition• Air Defense• Air Defense Fire Control• Air Traffic Control
MMR
SOF LCMR Army LCMR
10IDGA Sensors Nov 06 (10) Unclassified11 OCT 07 . Wittstruck (10)
The Path Forward
11IDGA Sensors Nov 06 (11) Unclassified11 OCT 07 . Wittstruck (11)
Assumptions used in Technology Assessment
Objective: To establish a working template to assess various device technologies for a power transmitter used in different system requirements.
• Solid-state phased array system• Output power per element: 25W• Mode of operation: CW and Pulsed • Final performance can be scaled
• Estimation of baseplate temperature needed to maintain PA MMIC(s) of different technologies; leading in cooling requirements
• For a particular technology, overall system DC conversion efficiency and I2R distribution loss also to be considered to assess its advantage; trade-off should be noted
12IDGA Sensors Nov 06 (12) Unclassified11 OCT 07 . Wittstruck (12)
Comparison of Technology for S-Band PAGaAs HV-GaAs GaN/SiC GaN/SiC-2 SiC
PHEMT PHEMTHEMT -
consv pwr HEMT -high pwr density MESFET
RF Pout (W) 25 25 25 25 25Gain (dB) 20 20 16 18 10Driver RF Pout required (W) 0.4 0.4 1.0 0.6 4.0Vbias (V) 9 25 40 48 48number of MMICs for Pout and gain 2 1 1 1 2+1Power density, W/mm, (HV-GaAs -estimated) 0.8 2.4 5.0 8.0 4.0Gate length (um) 0.25 0.35 0.35 0.35 0.80Gate periphery required (mm) 31 10 5 3 6PAE %, (pwr MMIC only), (HV-GaAs -estimated) 35 45 45 50 12Idc total (A), (pwr MMIC only) 7.94 2.22 1.39 1.04 4.34Junctn Tmax, C ( to maintain during operation) 150 200 200 230 230
Pdc diss, W (Pdc - Prf) 46.4 30.6 30.6 25.0 183.3Heat disspation / mm 1.5 2.9 6.1 8.0 29.3Temperature rise, C 88 173 80 104 164
Max. base plate temp allowed to maintain Pout 62 27 120 126 66
Pdc diss, W (Pdc - Prf) 9.29 6.11 6.11 5.00 36.67Heat disspation / mm 0.15 0.23 0.05 0.04 0.56Temperature rise 17.67 27.21 1.32 1.04 6.25
Max. base plate temp allowed to maintain Pout 132 173 199 229 224
Voltage Conversion Eff. (from 48V DC), estimates 67 81 90 90 95I*R Losses (relative to lowest, 1) 7.62 2.13 1.33 1.00 4.17
Final system power conver. includes: base plate temp, Voltage conversion, I2R loss for the array
TRL 9 5 3 - 4 3 5Ready for prototype MMICs now now FY06 FY07 nowAvail in systems, time depends on MTTF reqt now FY07 FY08 FY09 FY07
Parameters
CW case
Pulsed case (20% Duty cycle)
System Considerations
Technology Maturity
13IDGA Sensors Nov 06 (13) Unclassified11 OCT 07 . Wittstruck (13)
• Super heterodyne receiver architecture/concept- Theory was developed for CW RF- Doppler or information detection achieved by frequency domain filtering
• But, most modern Radar are pulsed Radar- Use multiple pulses- Increase transmission power- Require very high SFDR- Require super oscillators…
- Limited Performance:- Doppler-range ambiguity
Conventional Radar:
“There has been no significant change in Doppler Radar front-end architecture/concept since World-War II. The only difference in modern radar is the digital electronics for signal processing.”
LNA
RF in
LO
LF A/DIF
Skolnik
The Philosophy of Radar Design
14IDGA Sensors Nov 06 (14) Unclassified11 OCT 07 . Wittstruck (14)
DARPA Funded Seeding Efforts at Army Research Lab:
• Investigate the MicroDoppler signature- Theoretical modeling and simulation
- MicroDoppler detection - Noise analysis
• Study the experimental feasibility of interferoceiver- Fiber recirculation loop experiment- Technology survey
RF-Photonic Interferoceiver For MicroDoppler Radar
15IDGA Sensors Nov 06 (15) Unclassified11 OCT 07 . Wittstruck (15)
RF - Photonic Correlation Receiver for Channelizer Concept
True time domain self correlation produced by the fiber recirculation loop
filter
Fourier Transform
Self-correlation data in
Laser Modulator 1x2
φ
λ
RFin
t1
EDFA
Optical Amplifier
Coupler
t2
L1
L2
fiber
Interference combiner+sq law detector
A/D
)()()( nnntiExptfF
∆l
Astrophysicists are able to retrieve their signal 36dB below noise level!
(Joe Taylor)
16IDGA Sensors Nov 06 (16) Unclassified11 OCT 07 . Wittstruck (16)
Photonic Pulse Doppler Radar / Experimental
Laser
Laser
Modulator
Modulator
WDMφ
RFLO
λ1
λ2
RF inReceive antenna
Doppler out
System Design:
Pulse Doppler Radar:
tTpulse
Trange
Optical Amplifier/absorber
CouplerWDM
17IDGA Sensors Nov 06 (17) Unclassified11 OCT 07 . Wittstruck (17)
Let’s Transition This Technology
So that the future RF Radar systems can:• Use single transmit / receive pulse
• Don’t worry about SFDR • Don’t worry about speed and bandwidth of A/D
• Ultra wide band and frequency agile
• Channelizing with extreme large number of channels (large bandwidth, high resolution)
• 1 Hz resolution micro Doppler detection
• Precise range and Doppler for long distance high speed target
• Detect small signal from the noise floor
18IDGA Sensors Nov 06 (18) Unclassified11 OCT 07 . Wittstruck (18)
BACKUP
19IDGA Sensors Nov 06 (19) Unclassified11 OCT 07 . Wittstruck (19)
RF-Photonic Interferoceiver
One pulse can determine Doppler Beating
Reflected
Original
SQUARE
LAW RF
RECEIVER
Optical FiberRecirculation
Loop
Optical FiberRecirculation
Loop
Both loops have the same length L n is the number of circulations
Interfering Amplitudes
Intensity Variation
Exp inL
cf E xp i
v
c
nL
cf{ } ' ( ) { ( ) } ( ) 1
2
d Exp iv
c
nL
cf E xp i
nL
cf c c { ( ) } ( ) { } '* ( ) . .1
2
20IDGA Sensors Nov 06 (20) Unclassified11 OCT 07 . Wittstruck (20)
RF-Photonic Correlation Receiver For Channelizer
Self-Correlation in time domain
Received RFOptical FiberRecirculation
Loop L1
Optical FiberRecirculation
Loop L2
Transfer
t ω
Time domain correlation spectrum analyzer:But A/D sampling a CW signal.
t
Again, not a true time domain correlation!
)()()()()()( ** FtAttdtAtAtAtf nnnn
21IDGA Sensors Nov 06 (21) Unclassified11 OCT 07 . Wittstruck (21)
True Correlation Receivers
BAnnnnn FtBtAtf );()()()( *
)()()()()()( ** FtAttdtAtAtAtf nnnn
True Time Domain Correlation
Self-Correlator
Received RF
Reference RF
Optical FiberRecirculation
Loop
t
t
Received RF
Optical FiberRecirculation
Loop: L1
Optical FiberRecirculation
Loop: L2
Transfer
Transfer
ω
ω
22IDGA Sensors Nov 06 (22) Unclassified11 OCT 07 . Wittstruck (22)
True Correlation Receiver
The Power of Time Domain True Correlation Receiver
Astrophysicists are able to be able to retrieve their signal 36dB below noise level! (Joe Taylor)
t
ωωo
Received signalf(ωt)
Reference (LO)
f(ωot)
For CW RF: Time domain
Frequency domainDoppler
Cannot get infowith short pulse
We need to do correlation for pulse RF!