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The Importance of Dirt in Radio-Frequency Testing and Spectrum Management
Jeffrey Schleher, PE and James R. Duffey, PhD
American Systems Leidos
2015 ITEA DEPS Directed Energy Symposium May 12-15, 2015 Las Vegas, NV
Distribution Statement A: Approved for public release; distribution is unlimited
Approved for public release
Topics
• RF Propagation Considerations
• Ground Reflection
• Impact
• Modeling and Simulation
• Reflection Measurement
• Ground Propagation Needs
• Conclusions
2
Approved for public release
Topic Test Importance To:
• Remote Sensing
• RF Communication
– All wireless activity
• RF Electronic Warfare
• Trafficability
• HPEM Directed Energy
3
Approved for public release
RF Propagation Considerations
• Direct Propagation
• Propagation Through Foliage, Walls and Buildings (Urban and Rural Environment)
• Multiple Reflections
• Diffraction Around Buildings and Hills
• Ground
– Propagation Into Ground
4
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Reflection Coefficient
5
ReflectionCoefficient
= D R
GroundElectrical
Properties
DispersionCurvature
GroundRoughness
Long, Radar Reflectivity of Land and Sea, Artech, 1983This and next slide complex equations in El-Shenawee and Miller:“Multiple-Incidence and Multifrequency for Profile Reconstruction of Random Rough Surfaces Using the 3-D Electrometric Fast Multipole Model, IEEE Geo and Remote Sensingv42,#11 Nov 2004
Penetration of the ground, with loss, and then reflection is not addressed here or in most modelsThe challenge, then, is to know ground electrical properties with depth.
• Simplified RF Reflection Equation
Approved for public release
Ground Reflectionor absorption, or penetration, and reflection
2 2 2
2 2 2
sin cos
sin cos
i i
TM
i i
n n
n n
2 2
2 2
sin cos
sin cos
i i
TE
i i
n
n
sin
sin
cos
cos
x y z
x y z
x y z
x y z
j t j k x j k y j k zinc
x i
j t j k x j k y j k zref
x TE i
j t j k x j k y j k zinc
y i
j t j k x j k y j k zref
y TE i
E e
E e
E e
E e
sin cos
sin cos
sin sin
sin sin
cos
cos
x y z
x y z
x y z
x y z
x y z
x
j t j k x j k y j k zinc
x i i
j t j k x j k y j k zref
x TM i i
j t j k x j k y j k zinc
y i i
j t j k x j k y j k zref
y TM i i
j t j k x j k y j k zinc
z i
j t j kref
z TM i
E e
E e
E e
E e
E e
E e
y zx j k y j k z
R, R,
2 (1 )R
o R
n j
INCEINCH
TE CaseTM Case REF INC
TEH H REF INC
TME E
i i
Einc
Eref
Etrans
Free Space
Vertical
z
x
2
r
o
n j
i i
Einc
Eref
Etrans
Free Space
Vertical
z
x
2
r
o
n j
i i
HincHref
Htrans
Free SpaceX X
X
Horizontal
2
r
o
n j
i i
HincHref
Htrans
Free SpaceX X
X
Horizontal
2
r
o
n j
R, R,
ETRHTR
rr
(1 )TR INC r
TME E e (1 )TR INC r
TEH H e
o o Rj j
For Vertical and Horizontal Polarization
6
Long, Radar Reflectivity of Land and Sea, Artech, 1983 Assuming dirt not magnetic, = 1Olhoeft, Elec. Mag. And Geo Properties for GPR, 7th Int’l Conf on GPR, 1998
• Complete Equations Including Polarization
Field Into slide
Field out of slide
Approved for public release
Relative Electrical Properties
7Kerr, Propagation of Short Radio Waves, MIT Radiation Laboratory Series, vol 13, 1951, p. 398
Medium ’ ”
Sea water
Distilled water
Fresh-water lake
Very dry sandy loam
Very wet sandy loam
Very dry ground
Moist ground
Arizona sand
Austin TX Soilvery dry
3 m- 20 cm
3.2 cm
1 m
9 cm
9 cm
1 m
1 m
3.2 cm
3.2 cm
4.3
12
10-3 - 10-2
0.03
0.6
10—4
10-2
0.10
0.0074
S/m
80
67
80
2
24
4
30
3.2
2.8
774
23
0.06 – 0.6
1.62
32.4
0.006
0.6
0.19
0.014
wavelengthReal
Dielectric constantconductivity
ImaginaryDielectric constant
Approved for public release
Ground RoughnessRough Surfaces
Flat Surface Subsurface Electrical Properties Variation
White Sands Desert Pavement Moisture Intrusion Channels
8Rule of Thumb: If Δh < λ/8 sin φ, the surface is “flat” (ibid, Long, p.37)
Δh
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Soil Roughness Calculations
9
• Diagram used in accounting for roughness
El-Shenawee and Miller:“Multiple-Incidence and Multifrequency for Profile Reconstruction of Random Rough Surfaces Using the 3-D Electrometric Fast Multipole Model, IEEE Geo and Remote Sensing, v42,#11 Nov 2004
• Referenced paper addresses a Government model (NSF) which helps determine if roughness matters in any particular test
Computing conductivity from dielectric constant
0 ” 2pfConductivity
Permittivity of free space Imaginary part ofdielectric constant
Frequency
0 = 8.854187817620... × 10−12 farads per meter
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Why Ground Bounce Matters
• Constructive & Destructive Interference of Direct and Ground Scattered Wave• Unexpected high fields
• Energy goes to unexpected locations• Safety issue in test – Fratricide issue in operations
Modeling in THP -5 is less loss than expected with out ground: Fast, REMCOM, SDRL A001:Dielectric Sensitivity Analysis v1.0, DETEC 12 SEP 0610
0 1000 2000 3000 4000 5000 6000 7000 8000 9000 10000
1000
900
800
700
600
500
400
300
200
100
0
Range (meters)
Height (meters)
-5 0 5 10 15 20 25
Excess Loss above Free Space (dB)
0 1000 2000 3000 4000 5000 6000 7000 8000 9000 10000
1000
900
800
700
600
500
400
300
200
100
0
Range (meters)
Height (meters)
-5 0 5 10 15 20 25
Excess Loss above Free Space (dB)
Very Dry Ground, 1000 MHz, Antenna Height 3m, APMSea Water 1000 MHz, Antenna Height 3m, APM
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Wave Interaction
• Diagram of RF constructive and destructive interference
-1.5
-1
-0.5
0
0.5
1
1.5
Direct
Scatter
Interferance
Direct
Scatter
40%
11
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Interference StructuresIn theory and field
Field Strength Differences WithDifferent Soil Types at 100m
Ground Reflection
SoilTypesEffectsIn THP
Field Test of W-band Wave InteractionHeating of Carbon Loaded Kapton
Ground Roughness Scattering
THP Calculations, Ground Dielectric Sensitivity Study IEEE-AP, Vol . 48, No. 2, April 2006, pg 45
ModelField Test
12
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Theory and Field Response
10 m
6 m
Narrow Band Threat Source – A’Pretest analysis with RF-PROTEC
Could use for the application slidePlacement of targets and sensors
Could use to show Reflection? InField Test
Direct Pulse Ground Close Rail Far Rail
Off Boresight Vertically Polarized B-dot
14
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Directed Energy Test and Evaluation Capability
DETEC
Propagation Environment Measurement (PEM)
• Recognized Ground Electrical Properties were a Requirement– Could not find a commercial
approach with promise and Reasonable cost
• Science and Technology Was Necessary– Reflection (Done with HSEP)
– Propagation Through Ground (To go)
• PEM Acquired (Done)– Atmospheric Measurement
Equipment for Refraction
– Sea Measurement Equipment for Roughness
15
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Measuring Soil Electrical Properties
• Dielectric Constant
• Conductivity
• Magnetic Permeability ( is = 1 ?)
• Roughness (somewhere > 10GHz dominates)
16
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Core Sample & 3-Months Method
Fort A.P. Hill Soil Permittivity and Conductivity Measurements for the Wide Area Airborne Minefield Detection Program, Adelphi MD, paper 2002
17
Approach used by Corp of Engineers in Iraq and Afghanistan
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DET S&T Approach
• HPM Soil Electrical Properties (HSEP) Science and Technology Project
• Purpose was to quickly and accurately obtain the electromagnetic properties of test range soils before, during, and after HPM testing
• To address these problems by conventional approach:– 3 to 6 months elapse between time samples are taken and time they are
measured, need to shorten this time to minutes or hours
– Sample can change physically and electrically from time sample is taken until it is measured; needs to be representative of soil at time HPM test is conducted
– in-field testing accomplishes this
– Quality of HPM testing suffers if properties of environment are unknown at time of testing – up to x3 changes in power density on target
– Quality of input to Test Hazard Prediction (THP) program forces “worst case” exclusion zones resulting in excessive test monitoring costs
18
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HPM Soil Electrical Properties (HSEP) S&T
• Phase I– Selected and demonstrated two
soil electrical property measurement technique• Micro-strip Resonators
• Time Domain Reflectometry
• Phase II– Calibrated resonators to known
standards
– Made measurements in field
• Kirtland
• Utah Test and Training Range
• WSMR
– ≈ 3 minutes/measurement at one resonant frequency
– Technique works on urban building material
19
Microstrip ring resonators:400 MHz, 900 MHz, 2500 MHz
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HSEP Testing and Application
20
442 MHz
1020 MHz
2.975 GHz
(front and back)
HSEP is used in the field at • WSMR• AFRL• Redstone TC• China Lake NAWC• NRL (CREW)
Frequency (Hz)
S 11
(dB
)
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How do I use Soil Electrical Properties?
• Calculate safety zones with real soil electrical property values using THP or Builder
• Frequency management input• Plan tests with predicted field
– Optimum placement of targets and sensors
• Assess when EW or HPM targets will be “shielded” by environment
• Application to counter mine operations– HSEP only reports first few cm of depth, depending on
frequency and soil moisture– Reflection but not propagation
21
10 m
6 m
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Models
• Test Hazard Prediction
– EMPIRE
• APM, RPO, TIREM, VTRPE, etc.
– RF-PROTEC
• Builder
– EMPIRE
• APM, RPO, TIREM, VTRPE, etc.
22
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Builder EW Planning
CREW Modeling from interactive scenario Builder NRL Promotional23
CIED Applications
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Shortfall: Propagation Through Soil
24
• Also CIED and Counter Mine applications
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Solution ConsiderationsAnalysis of Alternatives
25
Criteria• Frequency Resolution 100MHz• Frequency range 50MHz-2GHz• Vertical resolution 10cm• Horizontal resolution 1m• mS resolution undetermined
Geophex Ltd, Raleigh NC
Three Months Again2-3 m Horizontal Resolution
100cm vertical resolution
Core Samples + Q Cell Differential Transmission
Ground Penetrating Radar
• Other Approaches
Approved for public release
Conclusions
• Understanding radio-frequency propagation issues in military testing in E3, EW, spectrum management, communications, DE, and safety is essential
• Ground propagation effects are important to understanding overall propagation issues
• Understanding the ground electrical properties are critical in accounting for radio-frequency waves attenuated by, scattering from or adsorption in penetrated soil
• Determining ground electrical properties is difficult and time consuming leading DET S&T to establish an instrumentation program to quickly obtain these properties– Properties for surface reflection have been met– Propagation through soil remain a shortfall
26