alireza tabatabaeenejad, mariko burgin , and mahta moghaddam radiation laboratory

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Retrieval of Soil Moisture and Vegetation Canopy Parameters With L- band Radar for a Range of Boreal Forests Alireza Tabatabaeenejad, Mariko Burgin , and Mahta Moghaddam Radiation Laboratory Department of Electrical Engineering and Computer Science University of Michigan Ann Arbor, MI, USA

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Retrieval of Soil Moisture and Vegetation Canopy Parameters With L-band Radar for a Range of Boreal Forests. Alireza Tabatabaeenejad, Mariko Burgin , and Mahta Moghaddam Radiation Laboratory Department of Electrical Engineering and Computer Science University of Michigan Ann Arbor, MI, USA. - PowerPoint PPT Presentation

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Page 1: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Retrieval of Soil Moisture and Vegetation Canopy Parameters With L-

band Radar for a Range of Boreal Forests

Alireza Tabatabaeenejad, Mariko Burgin, and Mahta Moghaddam

Radiation LaboratoryDepartment of Electrical Engineering and Computer Science

University of MichiganAnn Arbor, MI, USA

Page 2: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Introduction (1/3)

Soil Moisture is of fundamental

importance to the study and

understanding of

Cycling of Water & Energy,

Runoff Potential, Flood Control

Weather and Climate

Geotechnical Engineering,

Soil Erosion

Agricultural Productivity,

Drought Monitoring

Human Health

(mosquito-transmitted diseases

in wet areas)

2/33

Courtesy of ESA

Page 3: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Introduction (2/3)

The need to monitor soil moisture on a global scale has motivated

the European Space Agency (ESA)'s Soil Moisture and Ocean

Salinity (SMOS) mission and the National Aeronautics and Space

Administration (NASA)'s Soil Moisture Active and Passive (SMAP)

mission.

3/33

Courtesy of ESACourtesy of JPL

Page 4: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Introduction (3/3)

In this work,

We study the radar retrieval of soil moisture, as well as

canopy parameters, in a range of boreal forests.

The forward model is a discrete scatterer radar model.

The retrieval is formulated as an optimization problem.

The optimization algorithm is a global optimization scheme

known as simulated annealing.

4/33

Page 5: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Outline

Forward Scattering Model for Forested Area

Inverse Model

Inversion of Model Parameters

Forested Area (Synthetic Data)

Forested Area (CanEx-SM10 Data)

Conclusion

5/33

Page 6: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Outline

6/33

Forward Scattering Model for Forested Area

Inverse Model

Inversion of Model Parameters

Forested Area (Synthetic Data)

Forested Area (CanEx-SM10 Data)

Conclusion

Page 7: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Forward Model: Introduction

7/33

Soil & forest parameters

Scattering coefficients

Frequency, incidence angle

ForwardModel

;f(X p)X

p

Page 8: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Forward Model: Forest Geometry

Forest Geometry

8/33

* S. L. Durden, J. J. van Zyl, and H. A. Zebker, "Modeling and observation of the radar polarizationsignature of forested areas," IEEE Trans. Geosci. Remote Sens., May 1989.

Forward Model: A general discrete scatterer radar model

by Durden et al.*

Page 9: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Forward Model: Scattering Mechanisms (1/2)

Canopy Layer

Trunk Layer

Ground

bg

bg

tgThe model identifies

4 distinct scattering

mechanisms:

b: branch

bg: branch-ground

tg: trunk-ground

g: ground

9/33

* S. L. Durden, J. J. van Zyl, and H. A. Zebker, "Modeling and observation of the radar polarizationsignature of forested areas," IEEE Trans. Geosci. Remote Sens., May 1989.

Forward Model: A general discrete scatterer radar model

by Durden et al.*

Page 10: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Forward Model: Scattering Mechanisms (2/2)

Forward Model: A general discrete scatterer radar model

by Durden et al.*

The total backscattered power, represented by the Stokes matrix, is the

sum of the powers from all contributing scatterers.

10/33

* S. L. Durden, J. J. van Zyl, and H. A. Zebker, "Modeling and observation of the radar polarizationsignature of forested areas," IEEE Trans. Geosci. Remote Sens., May 1989.

𝑀𝑡𝑜𝑡 = 𝑀𝑏 +𝑇𝑏𝑇𝑡𝑀𝑏𝑔𝑇𝑡𝑇𝑏 +𝑇𝑏𝑇𝑡𝑀𝑡𝑔𝑇𝑡𝑇𝑏 + 𝑇𝑏𝑇𝑡𝑀𝑔𝑇𝑡𝑇𝑏

branchcontribution

branch-groundcontribution

trunk-groundcontribution

groundcontribution

Page 11: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

11/33

Forward Model: Parameters

The forest floor is modeled as a rough dielectric surface with a layer of

nearly vertical dielectric cylinders (representing tree trunks) on top of it.

• The soil dielectric constant is related to the soil moisture via the soil type*

Branches are represented by a layer of randomly oriented cylinders.

The forward model uses properties of

• large and small branches (dielectric constant, length, radius, density,

orientation)

• leaves (dielectric constant, length, radius, density)

• trunks (dielectric constant, length, radius, density)

• soil (volumetric moisture content, roughness RMS height)

• canopy height

to characterize a forested area.

* N.R. Peplinski, F.T. Ulaby, and M.C. Dobson, “Dielectric properties of soils in the 0.3-1.3 GHz range,” IEEE Trans. Geosci. Remote Sens., vol. 33, no. 3, pp. 803-807, 1995.

Page 12: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Forward Model: Sensitivity

12/33

Sensitivity of several dBs to soil

moisture at L-band in the

presence of large amount of

vegetation

Less sensitivity to soil moisture

as soil moisture increases

Preserved dynamic range while

canopy height increases

Increase in trunk-ground

double bounce counterbalanced

by an increase in attenuation by

trunk layer as trunk density

increases.

Dielectric constants correspond to OJP trees

(CanEx-SM10) and allometric relationships

are hypothetical.

Page 13: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Outline

13/33

Forward Scattering Model for Forested Area

Inverse Model

Inversion of Model Parameters

Forested Area (Synthetic Data)

Forested Area (CanEx-SM10 Data)

Conclusion

Page 14: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

The forward model has too many parameters to allow inversion

14/33

Inverse Model: Allometric relations

Allometric relations can be based on actual measurements, for example

Allometric relations are used to

relate unknown parameters to each

other and reduce the overall number

of unknowns

Ideally, one or two stand parameters

can be used as kernels to describe

the entire forest stand

Page 15: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inverse Model: Simulated Annealing (1/2)

15/33

Simulated annealing uses an analogy between the unknown parameters

and particles in the annealing process of solids.

A small randomly-generated perturbation is applied to the current model

parameters.

If ΔL<0, the new state is accepted, otherwise it is accepted with probability

exp(-ΔL /T) → Metropolis criterion

This process is repeated at a sequence of decreasing temperatures.

Page 16: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inverse Model: Simulated Annealing (2/2)

16/33

Temperature

Current State

Last accepted point of the chain

Best state so far

Page 17: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inverse Model: Cost Function

Cost Function L

where X = state pq = polarizationf = frequencyθ = incidence angle

σ = calculated backscattering coefficients

d = measured backscattering coefficients

HH and VV polarizations components are used in the inversion

17/33

Page 18: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Outline

18/33

Forward Scattering Model for Forested Area

Inverse Model

Inversion of Model Parameters

Forested Area (Synthetic Data)

Forested Area (CanEx-SM10 Data)

Conclusion

Page 19: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Synthetic Data (1/4)

Sample inversion for a sample forest using synthetic data and

hypothetical allometric relationships at L-band for four unknowns

19/33

d=2.5 m, ρtr=0.72 #/m2, mv=0.25,

h=2 cm

Dielectric constants are from

CanEx-SM10 (for an OBS forest)

and allometric relationships are

hypothetical.

Accurate retrieval for all

unknowns (soil moisture,

trunk density, canopy height,

roughness RMS height)

Page 20: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Synthetic Data (2/4)

Sample inversion for a sample forest using synthetic data and

hypothetical allometric relationships at L-band for four unknowns

20/33

d=2.5 m, ρtr=0.72 #/m2, mv=0.25,

h=2 cm

Dielectric constants are from

CanEx-SM10 (for an OBS forest)

and allometric relationships are

hypothetical.

Accurate retrieval for all

unknowns (soil moisture,

trunk density, canopy height,

roughness RMS height)

Page 21: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Synthetic Data (3/4)

Sample inversion for a sample forest using synthetic data and

hypothetical allometric relationships at L-band for four unknowns

21/33

d=2.5 m, ρtr=0.72 #/m2, mv=0.25,

h=2 cm

Dielectric constants are from

CanEx-SM10 (for an OBS forest)

and allometric relationships are

hypothetical.

Accurate retrieval for all

unknowns (soil moisture,

trunk density, canopy height,

roughness RMS height)

Absolute error in d = 0 m

Page 22: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Synthetic Data (4/4)

Sample inversion for a sample forest using synthetic data and

hypothetical allometric relationships at L-band for four unknowns

22/33

Absolute error in h = 0.2 cm

d=2.5 m, ρtr=0.72 #/m2, mv=0.25,

h=2 cm

Dielectric constants are from

CanEx-SM10 (for an OBS forest)

and allometric relationships are

hypothetical.

Accurate retrieval for all

unknowns (soil moisture,

trunk density, canopy height,

roughness RMS height)

Page 23: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Outline

23/33

Forward Scattering Model for Forested Area

Inverse Model

Inversion of Model Parameters

Forested Area (Synthetic Data)

Forested Area (CanEx-SM10 Data)

Conclusion

Page 24: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Overview

The data are from CanEx-SM10 in June 2010.

Data acquisition included Old Jack Pine, Young Jack Pine, and Old

Black Spruce forests, located in Saskatchewan, Canada.

NASA/JPL UAVSAR flown on a Gulfstream III aircraft acquired large

swaths of fully polarimetric L-band measurements.

Soil moistures and roughness RMS height are unknowns.

The other forest parameters are assumed known from ground

measurement

24/33

Page 25: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Three forests

Old Jack Pine (OJP), Young Jack Pine (YJP), Old Black Spruce (OBS) forests

Old Jack Pine:

Columnar trees, dry and flat sandy

loam ground, densely covered

with dry lichen, which is

transparent at L-band

Young Jack Pine:

Pyramidally-shaped trees, very

dry and flat sandy ground with

short and sparse ground cover

Old Black Spruce:

Columnar coniferous trees,

wet loam ground complicated by

a non-uniform moss and organic

layer, water puddles, and bushy

understory

25/33

Page 26: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Measurement transects

Ground measurements included a transect of 100 m along which several

measurements were taken in ~10-m intervals.

26/33

Page 27: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Results for OJP

Inversion of soil moisture at L-band

Average error (bias) is -0.01

RMS error is 0.043 (6m12m)

27/33

Average error (bias) is -0.008

RMS error is 0.03 (18m36m)

mυi

σ0i

Σ σ0i = σ0

Page 28: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Results for YJP

Inversion of soil moisture at L-band

Average error (bias) is 0.014

RMS error is 0.02 (6m12m)

28/33

Average error (bias) is 0.015

RMS error is 0.022 (18m36m)

mυi

σ0i

Σ σ0i = σ0

Page 29: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Results for OBS

Inversion of soil moisture at L-band

Average error (bias) is 0.14

RMS error is 0.24 (6m12m)

29/33

Average error (bias) is 0.92

RMS error is 0.16 (18m36m)

Average error (bias) is 0.93

RMS error is 0.11 (18m36m)

Σ σ0i = σ0

mυ (□)mυi

σ0i σ0

i

Σ mυi = mυ (*)

Page 30: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Inversion of Model Parameters: Adding more unknowns

30/33

Adding canopy height and trunk density to the

unknowns (four unknowns) and cross-pol

backscattering coefficient to the measured data points

(three data points), the error in soil moisture would

be large (0.085 cm3/cm3 for OJP) due to

Unreliability of the cross-pol radar measurements

Adding only canopy height to the unknowns (three

unknowns) and using only co-pol data (two data points),

results in an RMS error of 0.025 cm3/cm3 in soil

moisture.

Page 31: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Summary and Conclusion (1/2)

31/33

L-band retrieval of under-canopy soil moisture as well as

other canopy parameters using radar data was

investigated.

Simulated annealing accurately retrieved soil moisture

from only a few data points. (synthesize data, four

unknowns, allometric relationships)

Inversion was successful for the OJP and YJP sites.

(CanEx-SM10 data, two unknowns)

Page 32: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Summary and Conclusion (2/2)

32/33

Error was large for the OBS forest mostly due to

small sensitivity of the forward model to soil moisture for

larger moisture values

possible inaccuracies in the forest parameterization

complex nature of the forest floor

L-band radar is capable of retrieving surface soil

moisture in high-biomass forests (such as OJP) where

the soil moisture information is mainly carried by the

trunk-ground scattering mechanism.

Page 33: Alireza Tabatabaeenejad,  Mariko Burgin , and Mahta Moghaddam Radiation Laboratory

Questions

33/33

Thank you for your interest.

Do you have any questions?

Further questions:

Alireza Tabatabaeenejad [email protected]

Mariko [email protected]

Mahta [email protected]