igarss11_mw_v2.ppt

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July 29, 2011 IGARSS 2011, Vancouver 1 A SIMULATION STUDY OF TOPOGRAPHIC EFFECTS ON POLSAR CLASSIFICATION OF FORESTS AND CROPS M. L. Williams 1 and T. L. Ainsworth 2 1 Cooperative Research Centre for Spatial Information 2 Remote Sensing Division, Naval Research Laboratory

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Page 1: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 1

A SIMULATION STUDY OF TOPOGRAPHIC EFFECTS ON POLSAR CLASSIFICATION OF

FORESTS AND CROPS

M. L. Williams1 and T. L. Ainsworth2

1Cooperative Research Centre for Spatial Information2Remote Sensing Division, Naval Research Laboratory

Page 2: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 2

Methodology• Assess the Effects of Underlying Topography on

Polarimetric Forest Backscatter Using Simulated Data• Estimate the Polarimetric Returns not Corrected by

Orientation Angle Compensations– Compare orientation-angle corrected data against forest returns

simulated over flat terrain

• Simulated Imagery Allows One to Tease Apart Forest Scattering Mechanisms – Direct canopy backscatter, ground-trunk interaction, canopy

attenuation, etc.

• Goal: Use the Analysis of Simulated Data to Develop Better Forest Scattering Models for PolSAR Imagery

Page 3: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 3

Forest Simulations Start With a Tree

Bare Vertical Trunk

Dead Primary Branches

Upper Crown

Model of a Scots Pine, ~18m in heightBased on Detailed Measurements

Lower Crown

Detail of the Crown

Primary and Secondary Branch Structures

Page 4: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 4

To Make a Forest

• Tree Branches Grow to Edge of Canopy Envelop – Upper Crown – Live Branches– Lower Crown – Dry Branches– Add Needles / Leaves

• Generate a Set of Unique Trees• Semi-Randomly Plant the Forest:

Page 5: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 5

Scene Generation

View from Radar Platform at Mid-track

• A realization of a random, sloped ground surface generated according to surface roughness, soil moisture and slope parameters.

• Ground surface covered by layer of random vegetation.

• A forest stand realized as a circular area populated by trees.

• Trees have a distribution of heights around the supplied mean value.

• Tree positions are determined by shuffling from an initially uniform grid, with a crown-overlap cost function.

• Red envelopes mark “living” pine crown, grey layer is “dry” timber.

• Each tree is unique and realized in detail for SAR simulation.

Page 6: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 6

SAR Simulator – PolSARproSim• Basic Simulations Performed with Stand-alone Version

of the PolSARproSIM Software– Coherent, polarimetric SAR simulator – Methodology documented within PolSARpro

• Five Basic Scattering Components – Signal attenuated by all vegetation layers

Direct Ground

Direct Short Vegetation

Direct Forest

Ground-Forest Backscatter

Ground / Short- Vegetation Return

Page 7: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 7

Scene Summary• Primary Characteristics

– Scots Pine forest - ~2600 trees• Relatively sparse canopy with large trunk structure

• Mean tree height: 18m

• Mean canopy radius: 2.6m

• Canopy attenuates radar signals

– Low vegetation ground cover• Weak scatterer, weak signal attenuation

– Moderately rough, moist ground surface

• Range and/or Azimuth Ground Slopes– Independent variables in this initial study

• Coupled Radar Scattering Components – Attenuation, Ground Slopes & Multiple Scattering

Page 8: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 8

Polarimetric Analysis• A Select Set of Polarimetric Descriptors:

• Orientation Angle: θ– Related to range(γ) and azimuth(ω) slopes– The complex phase of the RR-LL correlation (circular basis)

∀ α-angle: Average scattering mechanism – Surface: 0°, Dipole: 45°, Dihedral: 90°

• Double Bounce Scattering Strength– Dominant scattering mechanism in our (current) simulated forest– Arises primarily from ground-trunk interactions

• Circular Basis Correlations – |ρ4|: Reciprocal of orientation angle variance

• Magnitude of the RR-LL correlation • Independent of the underlying scattering mechanism

– |ρr|: Reciprocal of the shape variation • Relates to the variance of the effective scatterer shape• Depends explicitly on the scattering mechanism

( ) ( )( ) ( ) ( )φφγ

ωθsincostan

tantan

+−−=

Page 9: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 9

A SAR Image Realization L-band, 5 Meter Resolution

RGB Image: HH, HV, VV

• Forest covered central region• Low vegetation area surrounds forest• Range increases from left to right

HH HV VH VV

Page 10: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 10

α-angle Histograms

Range Slope: 0°, 1°, 2° & 4°

Rapid decrease of high α components between 0° & 2°

Azimuth Slope: 0°, 6°, 8° & 10°

No change until ~6° slope then a shift to lower α values

Page 11: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 11

With azimuth slope set to zero, the orientation angle does not depend on range slope.

0 0.2 0.4 0.6 0.8 10

200

400

600

800

1000

1200

1400

Ort Dispersion (ρ4)

\s_cov_p000_p000

\s_cov_m006_p000

\s_cov_m004_p000

\s_cov_m002_p000\s_cov_p002_p000

\s_cov_p004_p000

\s_cov_p006_p000

-40 -20 0 20 400

200

400

600

800

1000

Orientation (deg)

\s_cov_p000_p000

\s_cov_m006_p000

\s_cov_m004_p000

\s_cov_m002_p000\s_cov_p002_p000

\s_cov_p004_p000

\s_cov_p006_p000

Range Slopes in Grassy RegionsOrientation Angle & Correlation |ρ4|

Low orientation angle correlations without a strong dependence on range slope. Slightly lower for positive slopes.

Page 12: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 12

Grass Region Forest

Small range tilt reduces double bounce power in forest, but not in the grassy regions.

Range Slopes in Forest AreaDouble Bounce Power & Ground-Forest Component

Ground-Forest Component

The ground-forest multiple scattering accounts for the rapid drop of the double bounce backscatter.

-30 -25 -20 -15 -10 -5 0 50

500

1000

1500

2000

Double Bounce Power (dB)

\s_cov_p000_p000\s_cov_m006_p000

\s_cov_m004_p000

\s_cov_m002_p000

\s_cov_p002_p000

\s_cov_p004_p000\s_cov_p006_p000

-30 -25 -20 -15 -10 -5 0 50

200

400

600

800

1000

1200

Double Bounce Power (dB)

\gfs_cov_p000_p000\gfs_cov_m006_p000

\gfs_cov_m004_p000

\gfs_cov_m002_p000

\gfs_cov_p002_p000

\gfs_cov_p004_p000\gfs_cov_p006_p000

All tree trunks are perfectly vertical – not a good approximation.

Page 13: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 13

The orientation angle basically matches changes in azimuth slopes.

Azimuth Slopes in Grassy RegionsOrientation Angle & Correlation |ρ4|

Low correlation values imply poor estimates of orientation angles.

0 0.2 0.4 0.6 0.8 10

200

400

600

800

1000

1200

Ort Dispersion (ρ4)

\s_cov_p000_p000

\s_cov_p000_p002

\s_cov_p000_p004\s_cov_p000_p006

\s_cov_p000_p008

\s_cov_p000_p010

-40 -20 0 20 400

200

400

600

800

1000

Orientation (deg)

\s_cov_p000_p000

\s_cov_p000_p002

\s_cov_p000_p004\s_cov_p000_p006

\s_cov_p000_p008

\s_cov_p000_p010

Page 14: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 14

-30 -25 -20 -15 -10 -5 0 50

200

400

600

800

1000

1200

1400

1600

Double Bounce Power (dB)

\s_cov_p000_p000

\s_cov_p000_p002

\s_cov_p000_p004\s_cov_p000_p006

\s_cov_p000_p008

\s_cov_p000_p010

Grass Region Forest

Small azimuth tilts allow ground-trunk scattering, only larger slopes reduce double bounce power in forest.

Azimuth Slopes in Forest AreaDouble Bounce Power

Ground-Forest Component

The ground-forest multiple scattering component accounts for double bounce changes with azimuth slope.

Tree trunk forward scattering is not limited to specular directions.

-30 -25 -20 -15 -10 -5 0 50

200

400

600

800

1000

1200

Double Bounce Power (dB)

\gfs_cov_p000_p000\gfs_cov_p000_p002

\gfs_cov_p000_p004

\gfs_cov_p000_p006

\gfs_cov_p000_p008\gfs_cov_p000_p010

Page 15: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 15

The orientation angle basically matches changes in azimuth slopes.

Azimuth Slopes in Forest AreaOrientation Angle & Correlation |ρ4|

Higher correlation values in forest area imply good estimates of the orientation angles.

0 0.2 0.4 0.6 0.8 10

500

1000

1500

2000

Ort Dispersion (ρ4)

\s_cov_p000_p000\s_cov_p000_p002

\s_cov_p000_p004

\s_cov_p000_p006

\s_cov_p000_p008\s_cov_p000_p010

-20 -15 -10 -5 0 50

200

400

600

800

1000

1200

1400

Orientation (deg)

\s_cov_p000_p000\s_cov_p000_p002

\s_cov_p000_p004

\s_cov_p000_p006

\s_cov_p000_p008\s_cov_p000_p010

Page 16: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 16

Full SAR Simulation

Azimuth Slopes in Forest AreaOrientation Angle

Orientation angle estimates from full SAR simulation closely matches the orientation angles of the strong ground-forest scattering component.

The ground-forest induced orientation angle shows low variance (high correlations) independent of azimuth slope.

The orientation angle variance from the full simulation increases with increases in the azimuth slope.

-20 -15 -10 -5 0 50

200

400

600

800

1000

1200

1400

Orientation (deg)

\s_cov_p000_p000\s_cov_p000_p002

\s_cov_p000_p004

\s_cov_p000_p006

\s_cov_p000_p008\s_cov_p000_p010

-20 -15 -10 -5 0 50

500

1000

1500

2000

Orientation (deg)

\gfs_cov_p000_p000\gfs_cov_p000_p002

\gfs_cov_p000_p004

\gfs_cov_p000_p006

\gfs_cov_p000_p008\gfs_cov_p000_p010

Ground-Forest Component

Page 17: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 17

Full SAR Simulation

Azimuth Slopes in Forest AreaScatter Shape Variation

The Shape Variation reflects inherent changes to the polarimetric scattering.

Even after orientation angle compensation, once the azimuth slopes exceed ~6°, the ground-forest scattering component changes character.

The double bounce scattering, probably generated from ground-trunk interactions, is greatly reduced.

This change in Shape Variation is consistent with the α-angle changes due to azimuth slopes shown earlier.

Ground-Forest Component

-1 -0.8 -0.6 -0.40

500

1000

1500

2000

2500

3000

3500

Shape Variation (ρab)

\gfs_cov_p000_p000

\gfs_cov_p000_p002

\gfs_cov_p000_p004\gfs_cov_p000_p006

\gfs_cov_p000_p008

\gfs_cov_p000_p010

-1 -0.5 0 0.5 10

200

400

600

800

1000

Shape Variation (ρab)

\s_cov_p000_p000

\s_cov_p000_p002

\s_cov_p000_p004\s_cov_p000_p006

\s_cov_p000_p008

\s_cov_p000_p010

Page 18: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 18

Grassy Region

Major Forest Scattering Components

Forest scattering, at least for our simulated Scots Pine forest, is almost completely specified by the Direct Forest (blue) and the Ground-Forest (green) scattering components.

The cyan curve, the combination of Direct Forest and Ground-Forest scattering, almost exactly matches the Full Scattering curve (red).

Forest Returns

-30 -25 -20 -15 -10 -5 0 50

500

1000

1500

Double Bounce Power (dB)

.\dfs_cov_p000_p000.tla

.\gfs_cov_p000_p000.tla

.\s_cov_p000_p000.tla

Mixed

Page 19: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 19

Major Forest Scattering Components

The Full Orientation Angle Correlation matches the Correlation formed from the Direct Forest and Ground-Forest scattering components.

Similarly, the Full Shape Variation reflects the combination of the Direct Forest and Ground-Forest scattering.

0 0.2 0.4 0.6 0.8 10

1000

2000

3000

4000

5000

6000

7000

Ort Dispersion (ρ4)

.\dfs_cov_p000_p000.tla

.\gfs_cov_p000_p000.tla

.\s_cov_p000_p000.tla

Mixed

-1 -0.5 0 0.5 10

500

1000

1500

2000

2500

3000

Shape Variation (ρab)

.\dfs_cov_p000_p000.tla

.\gfs_cov_p000_p000.tla

.\s_cov_p000_p000.tla

Mixed

Page 20: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 20

Preliminary Conclusions (1)

• Results Based on a Single Forest Simulation

– Relatively light canopy attenuation

– Sparse forest – typical of Scots Pine

• Known Defects in the Tree Realizations

– All tree trunks aligned perfectly vertical

– One can design trees with randomly angled trunks

• Only Investigated Polarimetric Variations with Ground Slope

– Wider variety of forest parameters needed

– Adjust relative weighting of canopy attenuation, direct ground scattering, tree architecture, etc.

• Simulations May Produce Artificial Artifacts Not Seen in Scenery

– Blind use or application of software may be misleading

Page 21: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 21

Preliminary Conclusions (2)• Both Range and Azimuth Slopes Reduce Double Bounce Ground-

Trunk Scattering in this Forest– Both orientation angle correlation and shape variation indicate inherent

changes in polarimetric scattering due to topographic slopes

• Orientation Angle Compensation Does Not Remove All Topographic Effects on SAR Polarimetry

• The Large Number of Forest Parameters May Limit Full Investigation – Tree architecture, relative ground / canopy scattering strength, and

canopy attenuation may be the important variables

Page 22: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 22

Background

Page 23: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 23

Volume of Spheroid Scatterers• Assuming a cloud of spheroids for volumetric

canopy scatterers, characterized by independent parameters: size, shape and orientation.

O

X

Y

Z

N)cos,sinsin,cos(sin θφθφθ

φ

θiθ

)cos,0,(sin ii θθ)0,1,0(

)sin,0,cos( ii θθ−

Each elementary scatterer features a body of revolution w.r.t. the symmetric axis, ON.

( )( )

− ββ

ββψ

ψββββ

cossin

sincos

0

0

cossin

sincos

b

a

S

S

The projected symmetry axis on the polarization plane is oriented towards angle β;

The local incidence angle w.r.t. the symmetry axis is ψ;

The principal scattering components are Sa and Sb.

Page 24: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 24

Circular Polarization Representation• Oriented targets can be clearly expressed in the

circular polarization basis– Mean orientation angle from the phase of RR-LL– Similar to circularly polarized weather radar analysis

222

4

1baLLRR SSSS −==

222

4

1baLRRL SSSS +==

β42*

4

1 jbaLLRR eSSSS −−=

( ) ( ) β2**

4

1 jbabaRLRR eSSSSSS −+−=

( ) ( ) β2**

4

1 jbabaRLLL eSSSSSS +−=

If β and ψ are separable,

Advantage: Orientation parameters readily separable as phase terms.

( ) 044

44 4cos βββ ρββ jjj eee −−− ≡−=

*22

*22

2

2

Re2

Re2

baba

baba

ba

ba

SSSS

SSSS

SS

SSCDR

++

−+=

+

−=

022

2

22

*22Im2

ββ ρρρ jr

j

baba

baba

x eeSSSS

SSjSS−− ≡

+−

+−=

Symmetric distribution Orientation

dispersionMean orientation angle

Independent of orientation 0: sphere 1: dipole

Relates to both shape variation and orientation dispersion

Page 25: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 25

Orientation Distribution• The orientation angle is close to a von Mises

distribution

0,0

cos

0 )(2

1)(

===

βθβκ

κπβ e

If

Established a relation between ρ2 and ρ4.The orientation parameters, mean and dispersion, can be determined and removed, which leaves only scatterer shape information.

Page 26: IGARSS11_MW_v2.ppt

July 29, 2011 IGARSS 2011, Vancouver 26

Physical Parameters Retrieval• It is then straightforward to solve the principal

components from orientation compensated data

• Theoretically, the solution works for a single volume scattering mechanism and homogenous targets, resolving parameters:

( )*222Re2 RLRRRRRLa SSSSS ++=

( )*222Re2 RLRRRRRLb SSSSS −+=

( )*22* Im2 RLRRRRRLba SSjSSSS +−=

( )22

ba

*ba

ab

SS

SSeℜ=ρ

2

2

b

a

S

Sr =

We get mean shape and shape variation.

Size

Shape

Orientation