The Radiation Laboratory
Dec 21, 2015
The Radiation Laboratory
The Radiation Laboratory
Outline:Outline:
MotivationMotivation
Detection of targets camouflaged under foliage using Detection of targets camouflaged under foliage using multi-frequency, -polarization, -incidence angle multi-frequency, -polarization, -incidence angle SAR/INSAR sensors. SAR/INSAR sensors.
Physics-based scattering and propagation modeling of Physics-based scattering and propagation modeling of clutterclutter
Model reduction (extraction of channel parameters)Model reduction (extraction of channel parameters)
Scattering models for hard targets under trees Scattering models for hard targets under trees
High resolution SAR/INSAR image simulatorHigh resolution SAR/INSAR image simulator
3-D SAR at MMW for target detection and identification 3-D SAR at MMW for target detection and identification
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MotivationMotivation
A reliable approach for detection and identification of A reliable approach for detection and identification of targets camouflaged under foliage with an acceptable false targets camouflaged under foliage with an acceptable false alarm rate and probability of detection has not yet been alarm rate and probability of detection has not yet been developed.developed.
Due to the complexity of the problem, i.e.Due to the complexity of the problem, i.e.
Signal attenuation, phase-front distortion, poor signal-Signal attenuation, phase-front distortion, poor signal-to-clutter ratio, etc., single sensor approaches (optical, IR, to-clutter ratio, etc., single sensor approaches (optical, IR, radar) do not produce satisfactory results.radar) do not produce satisfactory results.
“ “Capable sensors” operating in diverse modality in Capable sensors” operating in diverse modality in conjunction with novel algorithms can drastically enhance conjunction with novel algorithms can drastically enhance FAR and PD.FAR and PD.
Polarization diversity, Polarization diversity, Multi-frequencyMulti-frequency, Multi-static, , Multi-static, Multi-Multi-incidence angleincidence angle, Interferometric , Interferometric
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receiver
Phenomenology of Wave Phenomenology of Wave Scattering & Propagation In ForestScattering & Propagation In Forest
Forest is a complex random medium composed of lossy Forest is a complex random medium composed of lossy scatterers arranged a semi-deterministic scatterers arranged a semi-deterministic
Foliage cause significant attenuation, scattering, field fluctuationFoliage cause significant attenuation, scattering, field fluctuation
To assess performance of radar sensors and target detection To assess performance of radar sensors and target detection algorithms phenomenology of EM wave interaction with foliage algorithms phenomenology of EM wave interaction with foliage must be understood.must be understood.
Scattering from foliage (clutter)Scattering from foliage (clutter)
Target is in the close proximity of many scatterersTarget is in the close proximity of many scatterers
Distortion of phase front and the scattered field from targetDistortion of phase front and the scattered field from target
Signal level, fluctuations, polarization state, Signal level, fluctuations, polarization state,
impulse response, spatial coherence etc. depend on:impulse response, spatial coherence etc. depend on:
Tree densityTree density
Tree typeTree type
Tree height and structureTree height and structure
Satellite
UAV
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3D Tree Generation
Lindenmayer systems allow generation of complex tree structure using only a few parameters
An algorithm based on self-similarity
Gross structure: columnar, excurrent, decurren
Biophysical parameters include tree height, trunk diameter(dbh) and branching angle
Tree structure G = G(V,,P)
Axiom = X
Productions:
p1: X FF{-X}F{++X}F{+X}{-X}
p2: F FF
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• Tree Type: Coniferous and Deciduous• Inclusion of Botanical Information
– Tapering in Length and Diameter*Law of conservation of cross section
area
– Stochastic Processing– Leaf Arrangement
• Computer Implementation– Tree DNA generation and structure
visualization• Forest stand generation and visualization
(scaling and view angle)
Red Mapler02 = ra
2 + rb2
r0
rarb
Red Pine
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The Radiation Laboratory
Put Matts stuff hereFractal tree details
GUIStill scenario
Movie
Tree generation graphical user interface
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Scene Generation and VisualizationScene Generation and Visualization
Land coverLand cover
DEMDEM
Tree stand Tree stand placementplacement
Vehicles, Vehicles, transmitter, transmitter, and receiver and receiver placementplacement
The Radiation Laboratory Propagation & Scattering Model for Forest Canopies
• Scattering from discrete scatterersScattering from discrete scatterers- Trunk: stratified dielectric cylinder- Trunk: stratified dielectric cylinder- Branch: homogeneous dielectric cylinder- Branch: homogeneous dielectric cylinder- Leaf: dielectric disk or needle- Leaf: dielectric disk or needle- Ground: layered dielectric half-space- Ground: layered dielectric half-space
•• Single Scattering is invokedSingle Scattering is invoked
•• Four Scattering Mechanisms are includedFour Scattering Mechanisms are included
ES eik
0r
re
ik0ˆ k i
ˆ k s
rn
n1
N SnEoi
where Sn Snt Sn
gt Sntg Sn
gtgRough
Interface
0 0.05 0.1 0.15 0.2 0.25 0.30
2
4
6
8
10
12
14
16
h-pol.v-pol.
Hei
ght
Attenuation rate NP/m
The Radiation Laboratory Source or Observation Point Source or Observation Point in the Forestin the Forest
Near-field calculation is requiredNear-field calculation is required
Approximate analytical formulations for near-field Approximate analytical formulations for near-field scattering from branches and tree trunks are derive. scattering from branches and tree trunks are derive.
Coherent summation of scattered field from all tree Coherent summation of scattered field from all tree components. (Coherence is important at S-band and lower)components. (Coherence is important at S-band and lower)
Single scattering theory Interaction among tree structures are ignored.
E i
E s
E d
E rE r
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The Radiation Laboratory Backscattering Coefficient of Red Pine Forest
150 trees & 100 realization.
Density: 0.1/m2
30 40 50 60 70 80 90 100-60
-50
-40
-30
-20
-10
0
10
ovv
Frequency [MHz]
dB
MeanMax.Min.
30 40 50 60 70 80 90 100-50
-40
-30
-20
-10
0
10
ohh
Frequency [MHz]
dB
MeanMax.Min.
Red pineRed pine
Tree height: 15.3 mTree height: 15.3 m
Crown Height: 9.5 mCrown Height: 9.5 m
45
The Radiation Laboratory Time-Domain Response at a Time-Domain Response at a FDTD Grid PointFDTD Grid Point
0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2
x 10-7
-1.5
-1
-0.5
0
0.5
1
1.5
time [s]
Ey: h-pol.
With forestWithout forest
attenuation
0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2
x 10-7
-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
time [s]
Ex: v-pol.
With forestWithout forest
attenuation0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2
x 10-7
-0.4
-0.3
-0.2
-0.1
0
0.1
0.2
0.3
0.4
time [s]
Ez: v-pol.
With forestWithout forest
dispersion
Note: Small effect of forest
Frequency: 30MHz – 100MHz
10 trees are considered.
Dielectric constants: 21.7 + i14.6 for branch
9.8 + i1.7 for ground.
Height of tree: 15m, Diameter of trunk: 22cm.
45o Incidence angle.
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Time-domain ResponseTime-domain Response Observation point is 1m above the ground inside a pine forest.Observation point is 1m above the ground inside a pine forest.
v-pol. wave is incident at v-pol. wave is incident at 4040oo, and BW 1GHz (, and BW 1GHz (11GHz – GHz – 22GHz).GHz).
30 40 50 60 70-0.4
-0.2
0
0.2
0.4
0.6Free SpaceForest Channel: Mean field
Time[ns]
V/m
Ez
30 40 50 60 70-0.4
-0.2
0
0.2
0.4
0.6
Time[ns]
[V/m
]
Free SpaceForest Channel: Total field
V/m
Time[ns]
Ez
Severe distortion due to trees
& Dispersion
The Radiation Laboratory Interaction of Foliage and Target Hybrid Interaction of Foliage and Target Hybrid Frequency/Time-Domain SimulationsFrequency/Time-Domain Simulations
1.1. Using the forest model, calculate time domain response of several Using the forest model, calculate time domain response of several trees in the proximity of the target at FDTD grids on a box (excitation).trees in the proximity of the target at FDTD grids on a box (excitation).
h-pol. or v-pol.
2. Using FDTD, compute scattering from the target on the same grid Using FDTD, compute scattering from the target on the same grid points.points.
including all interactions
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3. To calculate the interaction between the target and the forest, reciprocity theorem is used. After exchanging observation & source points, use the previously calculated scattering property of the forest to obtain the final backscattering result.
Observation point
Source point
exchanging
Note: Using this procedure, interaction between forest & target is taken account into up to first order.
Hybrid Frequency/Time-Domain Hybrid Frequency/Time-Domain Simulations (Cont.)Simulations (Cont.)
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Validation
A 2x2x2 FDTD mesh is used to model free space within the forest (in the absence of any vehicles).
The same problem is solved by a pure MoM code.
Results of the two methods are in excellent agreement.
(y)(z)
(x)
2x2x2 FDTD mesh and electric field component that is plotted in the figure on the right.
FDTD simulation parameters :
x = y = z = 0.3 m
t = 0.314 nsec
Validation of Hybrid Frequency/Time-Domain Modeling
A FDTD box around the
observation point
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Discretized HUMVEE for Discretized HUMVEE for FDTD AnalysisFDTD Analysis
x
y
z400
Ei
Bistatic Scattering From Bistatic Scattering From HUMVEEHUMVEE
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Current Distribution over the HUMVEECurrent Distribution over the HUMVEE
Preliminary Results
The Radiation Laboratory Field Distribution On the FDTD Box(2 GHz)
v-pol. incidenceh-pol. incidence
Note : Considerable distortion due to trees.
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Mean Field at receiver is of the form:Mean Field at receiver is of the form:
Functional to macromodel mean field should be of similar formFunctional to macromodel mean field should be of similar form such as Prony’s exponential series expansion:such as Prony’s exponential series expansion:
According to Foldy’s approximation According to Foldy’s approximation < < S S > in forward > in forward direction, remembering:direction, remembering:
Macromodeling of Field Macromodeling of Field Statistics – Mean FieldStatistics – Mean Field
jαβkCeE effθz/jkT
ieff wherecos
pqSk
NIm
2
0
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<ETvx>
Pine Forest - Mean Field
<EThy> Simulated Data
Macromodel
i = 45o
Prony’s order = 3
<ETvz>
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Standard deviation is a smooth function of f It is therefore possible to macromodel the standard deviation with a functional in the form of a Taylor series polynomial:
Model reduction: Field STD
std(Ethy)
std(Etvx)
std(Etvz)
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Spatial Correlation
-5 0 50
0.2
0.4
0.6
0.8
1h-pol.
Calculated1/(1+ ax)
a = 1.58
-5 0 50
0.2
0.4
0.6
0.8
1
v-pol.
Calculated1/(1+ ax)
a = 1.07
iE
Observation line
Note: Since observation line is inside the shadow region, field should be highly correlated.
Model Reduction: Spatial Correlation
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VV Polarization HH PolarizationDirection of Flight
Incr
easi
ng R
ange
0dBsm Point Target 0dBsm Point Target
Michigan SAR Image Simulator Geometry
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Future Works
1.1. Use physics-based model for generating synthetic multi-Use physics-based model for generating synthetic multi-modal data modal data
• Statistics of clutter scattering and channel (Monte Carlo Statistics of clutter scattering and channel (Monte Carlo simulations)simulations)
• Hard target interaction with foliage (model reduction)Hard target interaction with foliage (model reduction)
2.2. Improvement of Forest Model AccuracyImprovement of Forest Model Accuracy
• Including the effects of near-field multiple scattering among Including the effects of near-field multiple scattering among vegetation components.vegetation components.
3.3. Hard target model reduction (scattering centers)Hard target model reduction (scattering centers)
4.4. Implement hybrid foliage/hard target interaction.Implement hybrid foliage/hard target interaction.
5.5. Improve computation time: Parallel processingImprove computation time: Parallel processing
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.
Z
BA1
A2
V
H
R
R+²R
h
h: height of a particular pixel
H: height of the radar
sinsincoscosRHh
50 Km X-band
225 Km C-band Swath Width
Shuttle Radar Topography Mission