igarss11_wang_v2.ppt

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July 26, 2011 IGARSS 2011, Vancouver 1 INVESTIGATION ON THE ORIENTATION AND STRUCTURE PARAMETERS OF CANOPY USING POLSAR OBSERVATIONS Yanting Wang, Thomas Ainsworth and Jong-Sen Lee Remote Sensing Division Naval Research Laboratory

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Page 1: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 1

INVESTIGATION ON THE ORIENTATION AND STRUCTURE PARAMETERS OF CANOPY

USING POLSAR OBSERVATIONS

Yanting Wang, Thomas Ainsworth and Jong-Sen Lee

Remote Sensing DivisionNaval Research Laboratory

Page 2: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 2

Objectives• Radar polarimetry enables better characterization of the targets with

shape and orientation parameters in addition to the conventional radiometric information.

• Model based decompositions are commonly used to interpret PolSAR observations.

• Multiple volume scattering models have been proposed:– The Freeman-Durden Model: randomly oriented dipoles– The Yamaguchi Model: anisotropic dipoles– The Freeman 2-Component Model: random oriented spheroids– Recently, Neumann augmented a model of anisotropic spheroids for

application to interferometric polarimetry data

• Is wide variation expected on the shape and orientation properties for different canopy types?

• Is it possible to estimate the shape and orientation parameters from PolSAR observations?

Page 3: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 3

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 4: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 4

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 5: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 5

Circular Polarization Representation• The polarimetric system is redundant when modeling

spheroids: for example, co-polar powers RR=LL

• An underdetermined system – the correlation ρx is product of two components:

• For a known distribution type, ρ2 can be inferred from ρ4.– Uniform distribution– Cosine distribution– von Mises distribution

• Then the orientation parameters, both mean and dispersion, can be removed from the covariance matrix.

222

4

1baLLRR SSSS −==

022

βρρρ jrx e−=

Page 6: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 6

Orientation Distribution• The symmetric axis direction in 3-D: von Mises-

Fisher distribution

kkONONON

kkONON

k

k

ˆ)ˆ(

ˆ)ˆ(

ˆ

ˆ//

•−=

•=

ii θφθθθφθβ

coscossinsincos

cossintan

−=

ii θφθθθψ sincossincoscoscos +=

0

cos

)]cos(sinsincos[cos

)sinh(4

)sinh(4),(

=

−+

=

=

θθκ

φφθθθθκ

κπκ

κπκφθ

e

ef

Orientation distribution (β):

symmetric, zero mean

Incidence angle

distribution (ψ): shows same dispersion

Page 7: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 7

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 8: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 8

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

SS=ρ

2

2

b

a

S

Sr =

We get mean shape, r, and shape variation, Re(ρab).

Size

Shape

Orientation

Page 9: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 9

Forest Observations• Multi-frequency AIRSAR data from different forest regimes

TropicalRainforest[Guyana]Jun. 93

- Broad leaf- Thick foliage- Random branches

TemperateConifer[Germany]Jun. 91

- Needle leaf- Oriented branches

TemperateDeciduous[Michigan]Oct. 94

- Low biomass- Random branches- Leaf-off scenario

* Image source: Google Earth

Page 10: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 10

• The frequency contour at 50th percentile

– At C-band, we expect dominant scattering from leaves.

– The scatterer orientation is quite random, as shown in low ρ4.

– Rainforest: medium-low ρab, near-zero r broad leaf shape

– Conifer: lower ρab, elongated r thin column shape

– Deciduous: lower ρ4, very low ρab, elongated r random twigs

C-band Forest Observations

C-band

Blue: rain forest (Guyana)Black: conifer (Germany)Cyan: deciduous (Michigan)

Page 11: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 11

L-band Forest Observations• The frequency contour at 50th percentile

– Rainforest: very low ρ4, near-zero ρab, near-zero r random orientation and random shape (deeper penetration through thick foliage).

– Conifer: higher ρ4, negative ρab, elongated r thin column shape, anisotropic branches, substantial trunk response.

– Deciduous: increased ρ4, negative ρab substantial trunk response, mixed response from twigs, branches, and trunk.

– Varying mechanisms presented in the polarimetric response at different frequencies

L-band

Blue: rain forest (Guyana)Black: conifer (Germany)Cyan: deciduous (Michigan)

Page 12: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 12

Vegetation Observations• Agricultural fields may be

more homogeneous• AIRSAR Flevoland dataset

– Ground truth blocks for supervised classifications

C-band L-band

Page 13: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 13

stembranchy

dipole;random

uniformshape

sphere;broader

needle;thinner

Scatter plots @ 50th percentile, C-band

leafyAt C-band, scattering from leaves

– Reasonable separation with significant overlapping

Dipole shape: stembeans, grass, wheat;

Broad shape: forest, beet, potatoes;Thin column: lucerne (random),

rapeseed;Disk shape: peas

Page 14: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 14

Scatter plots @ 50th percentile, L-band

At L-band, scattering component from structure – good separation.

Anisotropic dipole: stembeans, lucerne;

Thin column: wheat;Broad shape: potatoes, beet, grass;Mixed structure: forest;Uniform structure: rapeseed, peas

dipole;random

uniformshape

stembranchy

sphere;broader

needle;thinner

leafy

Page 15: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 15

Potential Physical Characterization

• The contours demonstrate “orthogonal” dimensions along shape and orientation – no apparent coupling.

• Easier to define the divisions for classification.• Easier interpretation of target scattering.

• Feasibility of using simple, gridded divisions to initiate classification:– Demonstrated through supervised classification

experiments

Size

Shape

Orientation

Page 16: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 16

Classification [C-band]Supervised

Target Type Orientation Randomness

Shape Variation

Mean Shape

Ratio (dB)

Total Span (dB)

Bare Soil 0.25 ~ 0.50 0.7 ~ 0.8 -2 ~ -1 -26 ~ -22 Forest 0.05 ~ 0.15 0.1 ~ 0.2 -1 ~ 1 -20 ~ -16 Grass 0.15 ~ 0.25 0.0 ~ 0.1 1 ~ 3 -24 ~ -20 Wheat 0.25 ~ 0.50 0.7 ~ 0.8 1 ~ 3 -20 ~ -16 Lucerne 0.15 ~ 0.25 0.1 ~ 0.3 1 ~ 3 -22 ~ -18 Stem Beans 0.05 ~ 0.15 -0.1 ~ 0.1 1 ~ 3 -20 ~ -16 Beets 0.05 ~ 0.15 0.3 ~ 0.4 -1 ~ 1 -18 ~ -14 Potatoes 0.05 ~ 0.15 0.2 ~ 0.3 -1 ~ 1 -18 ~ -14 Rapeseed 0.15 ~ 0.25 0.5 ~ 0.6 1 ~ 3 -20 ~ -16 Peas 0.15 ~ 0.25 0.5 ~ 0.6 -1 ~ 1 -20 ~ -16

Supervised Wishart Classification Experimental Wishart Classification(with extra step of segmentation)

Page 17: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 17

Classification [L-band]Supervised

Target Type Orientation Randomness

Shape Variation

Mean Shape

Ratio (dB)

Total Span (dB)

Bare Soil 0.50 ~ 0.70 0.8 ~ 0.9 -5 ~ -3 -28 ~ -22 Forest 0.05 ~ 0.20 -0.2 ~ 0.0 -3 ~ -1 -16 ~ -12 Grass 0.50 ~ 0.70 0.2 ~ 0.4 0 ~ 1 -26 ~ -22 Wheat 0.50 ~ 0.70 0.2 ~ 0.4 -5 ~ -3 -24 ~ -20 Lucerne 0.50 ~ 0.70 -0.2 ~ 0.0 1 ~ 3 -24 ~ -20 Stem Beans 0.50 ~ 0.70 -0.2 ~ 0.0 1 ~ 3 -18 ~ -14 Beets 0.05 ~ 0.20 0.3 ~ 0.5 -1 ~ 2 -22 ~ -16 Potatoes 0.05 ~ 0.20 0.1 ~ 0.3 -1 ~ 2 -18 ~ -14 Rapeseed 0.20 ~ 0.40 0.7 ~ 0.8 -3 ~ -1 -22 ~ -16 Peas 0.20 ~ 0.40 0.5 ~ 0.7 -3 ~ -1 -18 ~ -14

Supervised Wishart Classification Experimental Wishart Classification(with extra step of segmentation)

Page 18: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 18

Unsupervised Classification• Initial segmentation with discrete boundaries is

feasible for agricultural crops. – Establish a database of the discrete boundaries; or– Build an unsupervised classification process.

Initial Segmentation: start with dense, discrete, gridded

divisions

ρ4 at 0.15, 0.25, and 0.5

ρab from -0.9 to 0.9 with 0.2 intervals

Primary divisions

Secondary divisions: mean shape ratio, pixel intensity

100+ initial divisions

Page 19: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 19

Unsupervised Classification• Merge classes during Wishart classification

– Maintain subtle variations amongst crop returns– Concentrate on shape variation and orientation

angle dispersion

Merge the secondary divisions based on inter-class Wishart

distance.

)(lnln XCXC 1mm−+−≈ trnnd

[ ])()(21

m1

nn1

m CCCC −− +≈ trtrdmn

From sample X to Cm:

Inter-class:

Secondary divisions: Merge if the classes are close, leaving 38classes for the AIRSAR Flevoland dataset

Primary divisions: merge only if• one of the classes has a small population; • the classes have comparable compactness; and • the classes are direct neighbors in (ρab, ρ4) space

Final result: 20 classes for the AIRSAR Flevoland dataset

Class centers: Cm, Cn, …

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July 26, 2011 IGARSS 2011, Vancouver 20

Unsupervised Classification

Re-colored UnsupervisedWishart ClassificationMap

Supervised Wishart ClassificationMap

Iterations not necessary, Wishart classification converges fast (pixel change < 10%)

C-band L-band

Page 21: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 21

Unsupervised Classification• Coniferous / Deciduous Forests

Sault Saint Marie, Lake Superior, Michigan

C-band, Pauli RGB Composition

Black: Low Backscatter, SPAN<-10 dBGray: SurfaceGreen: Deciduous ForestBlue: Coniferous ForestYellow: Mixed Type

Page 22: IGARSS11_WANG_v2.ppt

July 26, 2011 IGARSS 2011, Vancouver 22

Summary• An empirical retrieval of shape and orientation

parameters for volumetric scatterers– Volume scattering dominates – Orientation distribution: von Mises – Homogenous targets

• The shape and orientation parameters and size form “orthogonal” dimensions in the polarimetric space.– Application of discrete, gridded boundaries

• Different model parameters for different forest types• Different polarimetric response at C-band and L-band• The simple grid divisions were used to initiate Wishart

polarimetric classification, giving rise to an automated unsupervised PolSAR classification procedure based on scatterer shape parameters and orientation dispersion.