Data assimilation to improve retrievals of land surface ...

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Data assimilation to improve retrievals of land surface parameters Tristan Quaife (University of Reading, UK) December 2012 [email protected]

Transcript of Data assimilation to improve retrievals of land surface ...

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Data assimilation to improve retrievals of

land surface parameters

Tristan Quaife (University of Reading, UK)

December 2012

[email protected]

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MODIS:

Moderate Resolution Imaging Spectrometer

• Two in orbit (onboard

Terra and Aqua)

• Since 2000

• Daily global coverage

• 250m 1km resolution

• Various spectral channels

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Some definitions - BRF

• Bidirectional reflectance factor

– The ratio of the radiance reflected into a finite solid

angle and the radiance reflected into the same angle

(under the same illumination conditions) from a perfect

Lambertian reflector

– This is what is reported as “reflectance” from passive

optical sensors (MODIS, Landsat, LISS etc) which

observe the top of atmosphere radiance

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Some definitions - BRDF

• Bidirectional reflectance distribution function

– ratio of incremental radiance, dLe, leaving surface

through an infinitesimal solid angle in direction (v, v),

to incremental irradiance, dEi, from illumination direction

’(i, i)

1

)(

),()',( sr

dE

dLBRDF

i

e

Ω'

Ω'ΩΩΩ

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BRDF example

Modelled barley reflectance, v from –50o to

0o (left to right, top to bottom).

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BRDF example

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MODIS BRDF sampling

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Some definitions – spectral albedo

• Spectral albedo

– The integral of the BRDF, at one wavelength, over the

viewing hemisphere with respect to the illumination

conditions. Two commonly used forms:

2

,1

ΩΩΩ ;Ω dBRDF2DHR =

222

,1

2;2 ΩΩΩΩΩΩ ddBRDFdBHR =

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Some definitions – albedo

• Albedo (or “broadband” albedo)

– The spectral albedo integrated over the desired

wavelength range:

– p(λ) is the proportion of incoming radiation at the given

wavelength and α(λ) is the spectral albedo

dp

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From data to information...

• The key to understanding the remote sensing

signal is to understand how the target modifies the

EMR distribution

• To begin with, assume the canopy is filled with

randomly positioned ‘plate’ absorbers (i.e.

leaves)...

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0

Depth

, z

1-D plane-parallel semi-infinite turbid medium

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0

Depth

, z Ω δm

I0

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0

Depth

, z

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1-D Scalar Radiative Transfer Equation

• for a plane parallel medium (air) embedded with a

low density of small scatterers

• change in specific Intensity (Radiance) I(z,) at

depth z in direction with respect to z:

• Requires either numerical techniques or fairly

broad assumptions to solve

( )( )zJzI

z

zIse ,),(

,W+W-=

W¶km

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A [relatively] simple semi-discrete solution Gobron, N., B. Pinty, M. M. Verstraete, and Y. Govaerts (1997), A semidiscrete model for

the scattering of light by vegetation, J. Geophys. Res., 102(D8), 9431–9446,

doi:10.1029/96JD04013.

Single scattered

soil reflectance

Single scattered

canopy reflectance

Multiply scattered

reflectance (requires numerical solution)

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Clumping

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Shadowing

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Geometric optics

Shaded

crown Illuminated

crown

Illuminated

soil

Shaded

soil

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Operational models

• Probably the minimum model required to be

general enough to work for most vegetation types

requires some element of radiative transfer and

geometric optics

• However such models are typically very difficult

and/or time consuming to invert

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Kernel driven BRDF model

ISOTROPIC VOLUMETRIC GEOMETRIC

+ +

surface BRDF =

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f = kernel weight K = kernel value n = number of kernels

λ = wavelength ρ = BRF Ω = view geometry Ω' = illumination geometry

Kernel driven BRDF model

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Dominant scattering map

(near infra red):

Red = Geo

Green = Iso

Blue = Vol

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K is known for any given geometry, so if f can be determined this enables: •Calculation of integral terms (e.g. albedo) •Normalisation of data to common geometries •Higher level data processing (e.g. burn scars)

Kernel driven BRDF model

ρ=Kf y=Hx

H is known for any given geometry, so if y can be determined this enables: •Calculation of integral terms (e.g. albedo) •Normalisation of data to common geometries •Higher level data processing (e.g. burn scars)

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Kernel driven BRDF model - albedo

• Where a is a vector of (pre-computed) integrals of

the BRDF kernels

• N.B. α is a spectral albedo in this case

α=ax

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Formulation of H

H =

Kiso(Ω1; Ωʹ1) Kvol(Ω1; Ωʹ1) Kgeo(Ω1; Ωʹ1)

Kiso(Ω2; Ωʹ2) Kvol(Ω2; Ωʹ2) Kgeo(Ω2; Ωʹ2)

Kiso(Ω3; Ωʹ3) Kvol(Ω3; Ωʹ3) Kgeo(Ω3; Ωʹ3)

Kiso(Ω4; Ωʹ4) Kvol(Ω4; Ωʹ4) Kgeo(Ω4; Ωʹ4)

Kiso(Ω5; Ωʹ5) Kvol(Ω5; Ωʹ5) Kgeo(Ω5; Ωʹ5)

⁞ ⁞ ⁞

Kiso(Ωn; Ωʹn) Kvol(Ωn; Ωʹn) Kgeo(Ωn; Ωʹn)

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Formulation of y

y =

ρ(Ω1; Ωʹ1; λ)

ρ(Ω2; Ωʹ2; λ)

ρ(Ω3; Ωʹ3; λ)

ρ(Ω4; Ωʹ4; λ)

ρ(Ω5; Ωʹ5; λ)

ρ(Ωn; Ωʹn; λ)

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Formulation of x

x =

fiso(λ)

fvol(λ)

fgeo(λ)

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x = (HTR-1H)-1HTR-1y

• Formulation used for the MODIS BRDF/albedo product (MCD43)

• Requires an 16 day window

Least squares (over determined case)

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Observation errors

R = rI = r 0 0 …

0 r 0 …

0 0 r …

⁞ ⁞ ⁞

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MODIS band 2: NIR

MODIS data product (MOD43)‏

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MODIS data product (MOD43)‏

MODIS band 2: NIR

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MODIS data product (MOD43)‏

Backup inversion algorithm used

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MODIS data product (MOD43)‏

No inversion!

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Potential improvements

• Eliminate use of the backup algorithm

• Produce daily estimates of kernel weights

– to improve timing of events

– best estimates where no data

• Reduce noise in parameters

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Data assimilation

• A key weakness of the NASA algorithm is that the

inversions are not constrained in anyway by the

preceding inversion results

• This is a clear opportunity to apply data

assimilation techniques…

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Kalman filter

• Additional requirements:

– Dynamic model (M)

– Model covariance (P) and forcing (Q)

– Estimate of initial state

xa = x + K(y - Hx)

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For‏simplicity…

M = I = 1 0 0

0 1 0

0 0 1

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For‏simplicity…

P = pI = p 0 0

0 p 0

0 0 p

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Peculiarities of the system 1

• Each observation is a linear combination of all

state vector elements, and…

• …the dynamic model is not really dynamic

• Consequently small numbers of observations in

the analysis window will produce odd state

estimates (which still fit the observations well)

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Peculiarities of the system 2

• The values of the state elements are unitless and

not readily interpreted in terms of things we can

observe on the ground

– Sometimes qualitative analysis used

• Consequently validation of the state vector values

is more-or-less impossible and we have to resort

to comparing y and Hxa

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Example – reflectance data

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Example – retrieved kernel weights

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Example – predictions of BRF & albedo

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Example – predicted vs. observed BRF

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Example – retrieved kernel weights

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Example – predictions of BRF & albedo

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Example – predictions of BRF & albedo

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Example – predicted vs. observed BRF

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In‏the‏practical‏you‏will…

• Experiment with changing:

– P, Q, R

– The size of the analysis window

– The spectral channel & sensor

• Also there are data from two regions:

– Spain (nice, cloud free data)

– Siberia (sparse, cloudy data)

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Quaife and Lewis (2010) Temporal constraints on linear BRDF model parameters. IEEE TGRS

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Quaife and Lewis (2010) Temporal constraints on linear BRDF model parameters. IEEE TGRS

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EOLDAS

• European Space Agency Project to improve data

retrievals and inter-sensor calibration

• Weak constraint variational DA scheme using the

following cost function:

http://www.eoldas.info/

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EOLDAS examples

Lewis P, Gomez-Dans J, Kaminski T, Settle J, Quaife T, Gobron N,

Styles J & Berger M (2012), An Earth Observation Land Data

Assimilation System (EOLDAS), Remote Sensing of Environment.

Leaf Area

Index

Chlorophyll

Time

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