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12/10/2015 1/47
FOREST IN SAR IMAGES
A small introduction to forest in remote
sensing by radar
Elise Koeniguer
Elise.koeniguer@onera.fr
12/10/2015 2/47
Biomass estimation
Forest studies:
• Civil applications
• Defense applications
Detection of vehicles behind
forest
Applications
12/10/2015 3/47
C Thiel et al. Forestry 2006;79:589-597
Earth specific sites for BIOMASS mission preparation
System Parameters (Sensor)
Wavelength/Frequency (X, C, L, and P bands)
Polarization (HH, VV, and HV)
Incidence angle
Resolution
Pixel size ( different from resolution !)
Target Parameters (Ground)
Structure (size, orientation, and distribution of scattering surfaces)
Surface roughness (relative to wavelength)
Dielectric constant (moisture content)
Slope angle/orientation
12/10/2015 4/47
main parameters
12/10/2015 5/47
Radar bands
Low frequency –
P-band
resolution cell
structure and size ⇔ wavelength λ
The longer the wavelength, the greater the
sensitivity to the vertical structure of vegetation
6
one antenna
Measurement:
One complex
Coefficientantenna Image 1
i
j
1
S
Aim : 2 D imaging
Only absolute value
is used
10/12/2015 7/47
Amazon deforestation in 10 years as determined using L-band SAR data.
Left: Image of Amazon forest area acquired by JERS-1/SAR in 1996.
Right: Image of same area acquired by ALOS/PALSAR in 2006.
How does forest look like in a SAR image
Forest: high signal
10/12/2015 8/47
𝐸 𝑟
ℎ
𝐸 𝑟
𝑣
=
𝐽ℎℎ 𝐽ℎ𝑣
𝐽 𝑣ℎ 𝐽 𝑣𝑣
𝐸ℎ
𝑖
𝐸 𝑣
𝑖
Polarimetric transformation
Polarization ellipse
Polarimetry is sensible to:
• Geometrical information (roughness, branches orientations
• dielectric information (material, wet conditions)
A polarimetric radar image
Radar targets
Determinist / Non-determinist (Number of element per resolution
cell, “random” position)
9







vvvh
hvhh
ss
ss
S
H
V











vv
hv
hh
L
s
s
s
k 2
analysis of the polarimetric properties of electromagnetic
waves and the scatterers of these waves
the complete scattering
properties of a radar scatterer
can be determined
Animals make use of their
polarization-sensitive visual
systems
Degree of polarization: help for navigation
Detection of surfaces: water is an horizontal polarizer
Contrast enhancement: between any object and its
surroundings.
Polarimetry
Image 1
i
j
10/12/2015 10/47
Usual representation of a polarimetric image
The Pauli basis
2S
2
1
hV












 vVhH
vVhH
SS
SS
k











0
0
1
k











0
1
0
k











1
0
0
k
0 230
t/ha
Previous onera campaign: Guyana
12
Previous onera campaign: Nezer
10/12/2015 13/47
Monostatic depolarization
for Nezer forest (Landes France)
Forest radar UHF:
Depolarization/entropy presents good contrast over forest stands
© google map
Second order polarimetric parameters for forest SAR images
Example of second order polarimetric parameter image
 
kkT






vvvh
hvhh
ss
ss
S
2S
2
1
hV












 vVhH
vVhH
SS
SS
k
• As soon as three different parameters are available, they can be used
for a colored representation
10/12/2015 14/47
Alternative representations of a polarimetric image
Example : Freeman decomposition
• What do we know about a tree / forest in a POLSAR image ?
10/12/2015 15/47
Polarimetric signal for the forest
Range axis
shadow
Strong focused double bounce
Oriented components
10/12/2015 16/47
Some real examples
- Where is the range axis ?
- Why the double bounce echo is not exactly red?
10/12/2015 17/47
Polarimetric signal for the forest
18
Two antennas
Measurement:
two complex
coefficients
h
Antenna 2
Antenna 1
Image 1
i
j
Image 2
i
j
2
S
1
S
Aim : 3 D cartography
Interferometric image : InSAR
19
H
h
iobs
iinc
Combination of two radar measurements of the same
point on the ground, from slightly different angles
differences in phase related
to (R1-R2)
to the altitude at each position



2
2
2
1
*
21
2,1



2
1

 are two stochastic
complex signals
Interferometric coherence:
(Schwarz inequality)10 2,1  
■ The height h of the pixel is deduced from φ=arg()
■ The coherence level is deduced from |  |
Interferometry

φ
||
10/12/2015 20/47
Interfermetric image for the forest
||
φ
• What do we know about a tree / forest in a InSAR image ?
• Coherence level
• Mainly temporal decorrelation
• Not so high for low frequencies
• More linked to change of meteo conditions than wind
• Scattering phase center:
• somewhere in the forest.
• Linked to attanuation and density
10/12/2015 21/47
Interfermetric signal for the forest
22








 11
11
1
vvvh
hvhh
SS
SS
S 







 22
22
2
vvvh
hvhh
SS
SS
S















2212
1211
TT
TT
kkT
k
k
k †
†
2
1






2112
2222
1111
kkT
kkT
kkT













hv
vvhh
vvhh
P
s
ss
ss
k
1
11
11
1
2













hv
vvhh
vvhh
P
s
ss
ss
k
2
22
22
2
2
Image 1 Image 2
i
j j
i
Polarimetric Interferometry : POLINSAR
23
hH
vV
hV
Applications :
-coherence optimization for
the estimation of heights
- target analysis: how to get
the maximum information
- separation and
interpretation of different
heights


 


2211
12
)(
TT
T



22221111
2121
21 ),(


 


TT
T









2112
2222
1111
kkT
kkT
kkT
Coherence
matrices
3 x 3
• generalized coherence
POLINSAR – main parameters
• What do we know about a tree / forest in a POLInSAR image ?
• Coherence optimization
• Mainly temporal decorrelation
• Not so high for low frequencies
• More linked to change of meteo conditions than wind
• Scattering phase center:
• somewhere in the forest.
• Linked to attanuation and density
10/12/2015 24/47
POLINSAR signal for the forest
25
Existing Models:
 analytical models : Random Volume Over Ground model and inversion
[Treuhaft et al., 1996] Radio Science
 exact models
 descriptive models ex COSMO
Problems:
 The Random Volume Over Ground Model description is not suitable at P-
band or X-band
 Exact models : time consuming
 Descriptive modeling : very high numbers of entries for inversion
Modelling forest in POLINSAR
26
Vh
0i
e
veg
i
e 0
inversion
 ,, 0Vh
coherence
set predicted
by the model
0

The classical RVoG model : Random Volume over Ground
27
● attenuation: bad precision of the inversion for high frequencies (>C-band)
● importance of the precision on the estimation of the ground phase
● if differences between polarizations are too small, the linear regression is badly conditioned
)(
opt
),( 21 
opt
● the accuracy depends on the number of
samples used to compute the coherence.
● coherence optimization has to be used
carefully.
Limitations of RvoG
28
Vh
Litteral model (RVoG) descriptive model (Ex:COSMO)
very simple
more realistic
(cylinders at different
position,orientations)
Inversion
 ,, 0Vh
Analysis of
forest trends
not possible, or at least
numerical and very difficult
not possible
possible:
outputs by mechanism
outputs by scatterers
possible
litteral, POL, IN numerical, POL, INoutputs
description
[Treuhaft et al., 1996] Radio Science [Thirion, 2003] phD Thesis
Comparative analysis between two kinds of models
29
Litteral model (RVoG) descriptive model (Ex:COSMO)
Advantages
Drawbacks
attenuation expressed in dB/m is
overestimated by a factor of 2.
bad precision of the inversion for the
attenuation
not adapted to high densities.
description too simple for certain forest,
at certain frequencies
validated for several forest configurationssimple enough for inversion
does not enable the time-frequency
analysis
not adapted to high densities.
too many inputs for inversion
does not take into account group
effects
Comparative analysis of two kinds of models
10/12/2015 30
Further : tomography

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4-1 foret

  • 1. 12/10/2015 1/47 FOREST IN SAR IMAGES A small introduction to forest in remote sensing by radar Elise Koeniguer Elise.koeniguer@onera.fr
  • 2. 12/10/2015 2/47 Biomass estimation Forest studies: • Civil applications • Defense applications Detection of vehicles behind forest Applications
  • 3. 12/10/2015 3/47 C Thiel et al. Forestry 2006;79:589-597 Earth specific sites for BIOMASS mission preparation
  • 4. System Parameters (Sensor) Wavelength/Frequency (X, C, L, and P bands) Polarization (HH, VV, and HV) Incidence angle Resolution Pixel size ( different from resolution !) Target Parameters (Ground) Structure (size, orientation, and distribution of scattering surfaces) Surface roughness (relative to wavelength) Dielectric constant (moisture content) Slope angle/orientation 12/10/2015 4/47 main parameters
  • 5. 12/10/2015 5/47 Radar bands Low frequency – P-band resolution cell structure and size ⇔ wavelength λ The longer the wavelength, the greater the sensitivity to the vertical structure of vegetation
  • 6. 6 one antenna Measurement: One complex Coefficientantenna Image 1 i j 1 S Aim : 2 D imaging Only absolute value is used
  • 7. 10/12/2015 7/47 Amazon deforestation in 10 years as determined using L-band SAR data. Left: Image of Amazon forest area acquired by JERS-1/SAR in 1996. Right: Image of same area acquired by ALOS/PALSAR in 2006. How does forest look like in a SAR image Forest: high signal
  • 8. 10/12/2015 8/47 𝐸 𝑟 ℎ 𝐸 𝑟 𝑣 = 𝐽ℎℎ 𝐽ℎ𝑣 𝐽 𝑣ℎ 𝐽 𝑣𝑣 𝐸ℎ 𝑖 𝐸 𝑣 𝑖 Polarimetric transformation Polarization ellipse Polarimetry is sensible to: • Geometrical information (roughness, branches orientations • dielectric information (material, wet conditions) A polarimetric radar image Radar targets Determinist / Non-determinist (Number of element per resolution cell, “random” position)
  • 9. 9        vvvh hvhh ss ss S H V            vv hv hh L s s s k 2 analysis of the polarimetric properties of electromagnetic waves and the scatterers of these waves the complete scattering properties of a radar scatterer can be determined Animals make use of their polarization-sensitive visual systems Degree of polarization: help for navigation Detection of surfaces: water is an horizontal polarizer Contrast enhancement: between any object and its surroundings. Polarimetry Image 1 i j
  • 10. 10/12/2015 10/47 Usual representation of a polarimetric image The Pauli basis 2S 2 1 hV              vVhH vVhH SS SS k            0 0 1 k            0 1 0 k            1 0 0 k
  • 11. 0 230 t/ha Previous onera campaign: Guyana
  • 13. 10/12/2015 13/47 Monostatic depolarization for Nezer forest (Landes France) Forest radar UHF: Depolarization/entropy presents good contrast over forest stands © google map Second order polarimetric parameters for forest SAR images Example of second order polarimetric parameter image   kkT       vvvh hvhh ss ss S 2S 2 1 hV              vVhH vVhH SS SS k
  • 14. • As soon as three different parameters are available, they can be used for a colored representation 10/12/2015 14/47 Alternative representations of a polarimetric image Example : Freeman decomposition
  • 15. • What do we know about a tree / forest in a POLSAR image ? 10/12/2015 15/47 Polarimetric signal for the forest Range axis shadow Strong focused double bounce Oriented components
  • 16. 10/12/2015 16/47 Some real examples - Where is the range axis ? - Why the double bounce echo is not exactly red?
  • 18. 18 Two antennas Measurement: two complex coefficients h Antenna 2 Antenna 1 Image 1 i j Image 2 i j 2 S 1 S Aim : 3 D cartography Interferometric image : InSAR
  • 19. 19 H h iobs iinc Combination of two radar measurements of the same point on the ground, from slightly different angles differences in phase related to (R1-R2) to the altitude at each position    2 2 2 1 * 21 2,1    2 1   are two stochastic complex signals Interferometric coherence: (Schwarz inequality)10 2,1   ■ The height h of the pixel is deduced from φ=arg() ■ The coherence level is deduced from |  | Interferometry  φ ||
  • 20. 10/12/2015 20/47 Interfermetric image for the forest || φ
  • 21. • What do we know about a tree / forest in a InSAR image ? • Coherence level • Mainly temporal decorrelation • Not so high for low frequencies • More linked to change of meteo conditions than wind • Scattering phase center: • somewhere in the forest. • Linked to attanuation and density 10/12/2015 21/47 Interfermetric signal for the forest
  • 22. 22          11 11 1 vvvh hvhh SS SS S          22 22 2 vvvh hvhh SS SS S                2212 1211 TT TT kkT k k k † † 2 1       2112 2222 1111 kkT kkT kkT              hv vvhh vvhh P s ss ss k 1 11 11 1 2              hv vvhh vvhh P s ss ss k 2 22 22 2 2 Image 1 Image 2 i j j i Polarimetric Interferometry : POLINSAR
  • 23. 23 hH vV hV Applications : -coherence optimization for the estimation of heights - target analysis: how to get the maximum information - separation and interpretation of different heights       2211 12 )( TT T    22221111 2121 21 ),(       TT T          2112 2222 1111 kkT kkT kkT Coherence matrices 3 x 3 • generalized coherence POLINSAR – main parameters
  • 24. • What do we know about a tree / forest in a POLInSAR image ? • Coherence optimization • Mainly temporal decorrelation • Not so high for low frequencies • More linked to change of meteo conditions than wind • Scattering phase center: • somewhere in the forest. • Linked to attanuation and density 10/12/2015 24/47 POLINSAR signal for the forest
  • 25. 25 Existing Models:  analytical models : Random Volume Over Ground model and inversion [Treuhaft et al., 1996] Radio Science  exact models  descriptive models ex COSMO Problems:  The Random Volume Over Ground Model description is not suitable at P- band or X-band  Exact models : time consuming  Descriptive modeling : very high numbers of entries for inversion Modelling forest in POLINSAR
  • 26. 26 Vh 0i e veg i e 0 inversion  ,, 0Vh coherence set predicted by the model 0  The classical RVoG model : Random Volume over Ground
  • 27. 27 ● attenuation: bad precision of the inversion for high frequencies (>C-band) ● importance of the precision on the estimation of the ground phase ● if differences between polarizations are too small, the linear regression is badly conditioned )( opt ),( 21  opt ● the accuracy depends on the number of samples used to compute the coherence. ● coherence optimization has to be used carefully. Limitations of RvoG
  • 28. 28 Vh Litteral model (RVoG) descriptive model (Ex:COSMO) very simple more realistic (cylinders at different position,orientations) Inversion  ,, 0Vh Analysis of forest trends not possible, or at least numerical and very difficult not possible possible: outputs by mechanism outputs by scatterers possible litteral, POL, IN numerical, POL, INoutputs description [Treuhaft et al., 1996] Radio Science [Thirion, 2003] phD Thesis Comparative analysis between two kinds of models
  • 29. 29 Litteral model (RVoG) descriptive model (Ex:COSMO) Advantages Drawbacks attenuation expressed in dB/m is overestimated by a factor of 2. bad precision of the inversion for the attenuation not adapted to high densities. description too simple for certain forest, at certain frequencies validated for several forest configurationssimple enough for inversion does not enable the time-frequency analysis not adapted to high densities. too many inputs for inversion does not take into account group effects Comparative analysis of two kinds of models