abstract in the case of the application of the soil moisture and ocean salinity (smos) mission to...

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Abstract In the case of the application of the Soil Moisture and Ocean Salinity (SMOS) mission to the field of hydrology, the question asked is the following: how may the soil moisture retrieved from SMOS at the scale of 40 km be distributed at the hydrological scale of 1 km? To answer this question, the down- scaling scheme used in this study consists in linking local soil moisture to global signature in microwave band – the brightness temperature measured by SMOS – and to local surface temperature that provides information at the scale of 1 km – surface temperature is currently remotely sensed at this scale. The down-scaling technique is based on a scheme that was developed for distributing water storages in heterogeneously cleared large catchments. To apply this method to the field of remote sensing, a radiative transfer model is used to simulate microwave emissions at different scales from global scale (SMOS pixel) to local scale (one sub-pixel). First, soil moisture distribution inside SMOS pixel is linked to surface temperature distribution by a local filter based on the relationship between these two surface variables involved in a radiative process. This point is called the local constraint to the system. Second, soil moisture distribution is normalized so that the mean brightness temperature simulated by all sub-pixels is equal to SMOS brightness temperature. This point is called the global constraint. The general method is tested with a synthetic scene generated with a SVAT model coupled to the radiative transfer model. The results show a good distribution of local soil moisture within the generated SMOS pixel. Finally, the limitations of the down-scaling Conclusion The problem of distributing soil moisture within a SMOS pixel from SMOS observation at global scale and some information on the state and characteristics of the surface at local scale is not well constrained. The choice of estimating soil moisture distribution with surface temperature distribution is based on the following hypothesis: 'surface temperature varies quasi linearly with soil moisture in a given soil moisture range and in homogeneous surface conditions'. From this postulate, it is possible to formulate a local constraint function of two parameters and called the relative distribution constraint. The application of this constraint to the down-scaling problem reduces the dimension of the space of solutions from 1600 to 2. Two is also the number of independent global constraints that is possible to apply on the system: one at surface level and another at observation level. These global constraints may be used to calibrate successively both parameters of the relative distribution, the effective level parameter and the contrast parameter.The application of the down-scaling on a synthetic scene outlines the relevance of the approach. The heterogeneity of surface conditions that is likely to generate a systematic noise on distributed soil moisture is reduced and the spatial structure of generated soil moisture is well restituted. The sensitivity analysis shows a great robustness of the scheme towards uncertainties, which may be important, on local auxiliary information. However, this study shows that a limitation exists as concerned the determination of the contrast parameter when a noise is added on global observation. The multi-angular and bi-polarized capabilities of SMOS captor seem to be not sufficient for determining precisely the contrast of the relative distribution. I. Objective of the Study Distribution of surface soil moisture within a SMOS pixel by multi-spectral analysis II. Formulate 3 Constraints to the Distributed System III. Apply the Down-Scaling Scheme Surface Variables Random Generator Radiative Transfer Model (L band) SMOS global observati on LAI Soil Tempe rature Other Variables Generate a Synthetic Scene Algorithm Model Generated Soil Moisture Distributed Soil Moisture Results IV. Limitations Soil Moist ure Olivier MERLIN*, Ghani CHEHBOUNI, Yann Kerr, Philippe RICHAUME, Pierre GENTINE CESBIO, 18 Avenue Edouard Belin, Toulouse cedex 4, France * [email protected] Verify Primordial Hypothesis ‘Are local information obtained in other spectral bands (LAI, surface temperature) sufficient to distribute Soil Moisture given SMOS Observation?’ minimized SMOS Observation L band Local information in Optic et Thermal bands Resolution ~ 40 km Resolution ~ 1 km W W i W W W W f W W i i i i 1 SMOS BT f BT 1 2 1 1 1 f TB TB F f W W W W f W W SMOS i i i i Relative Distribution Constraint (C1) Surface Global Constraint (C2) Observation Global Constraint (C3) i i X f f W 1 0 Distributed Soil Moisture Level Distribution Parameter Variable whose space variability is linked to the space variability of surface temperature Contrast Distribution Parameter ‘Surface Temperature varies quasi linearly as a function of Soil Moisture in a specific range of Soil Moisture and in homogeneous Surface Conditions’ Sensitivity Analysis C ase SoilTem perature (K) LAI (%) SM O S O bservation (K) N oise 1 2 20 0 N oise 2 4 50 0 N oise 3 0 0 1 N oise 4 0 0 2 N oise 5 0 0 4 B A W (%) f1 C ase Viewing C onfiguration M ean Standard deviation M ean Standard deviation A 19.5 0 -3.0 0 N o N oise B 19.5 0 -3.0 0 A 19.5 0.0 -3.0 0.1 N oise1 B 19.5 0.0 -3.0 0.1 A 19.3 0.1 -2.7 0.5 N oise2 B 19.3 0.1 -2.9 0.4 W (%) f1 C ase View ing C onfiguration M ean Standard deviation M ean Standard deviation A 19.5 0 -3.0 0 N o Noise B 19.5 0 -3.0 0 A 19.5 0.3 -2.6 2.3 N oise3 B 19.5 0.1 -2.6 2.0 A 19.6 0.5 -3.0 2.5 N oise4 B 19.5 0.3 -2.9 2.2 A 19.5 1.1 -3.1 2.7 N oise5 B 19.5 0.6 -2.9 2.5 States signed by L band Surface States Measured States C3 C2 C1 Simulated Physical States Simulated Non-Physical States i i m i i m SMOS X T BT , , i i m i i m X T BT , , i i m i m i X T BT , , i i m SMOS X T BT , , i i m i m i X T W , , i i m i X T W , , i i m i i m i X T W , , i i m i i m X T W , , G G P 1 local RT local RT 1 global RT (G global ) (G local ) (F global ) (F local ) Radiative Transfer Layer (Model) C1 C2 Soil moisture distribution Projected soil moisture distribut ion Dynamic increment of contrast Contrast equal to zero (initialization) Adjust Global level k F Minimal value of global cost function C3 Distributed soil moisture (output) Application of Filter Surface Budget Model

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Page 1: Abstract In the case of the application of the Soil Moisture and Ocean Salinity (SMOS) mission to the field of hydrology, the question asked is the following:

AbstractIn the case of the application of the Soil Moisture and Ocean Salinity (SMOS) mission to the field of hydrology, the question asked is the following: how may the soil moisture retrieved from SMOS at the scale of 40 km be distributed at the hydrological scale of 1 km? To answer this question, the down-scaling scheme used in this study consists in linking local soil moisture to global signature in microwave band – the brightness temperature measured by SMOS – and to local surface temperature that provides information at the scale of 1 km – surface temperature is currently remotely sensed at this scale. The down-scaling technique is based on a scheme that was developed for distributing water storages in heterogeneously cleared large catchments. To apply this method to the field of remote sensing, a radiative transfer model is used to simulate microwave emissions at different scales from global scale (SMOS pixel) to local scale (one sub-pixel). First, soil moisture distribution inside SMOS pixel is linked to surface temperature distribution by a local filter based on the relationship between these two surface variables involved in a radiative process. This point is called the local constraint to the system. Second, soil moisture distribution is normalized so that the mean brightness temperature simulated by all sub-pixels is equal to SMOS brightness temperature. This point is called the global constraint. The general method is tested with a synthetic scene generated with a SVAT model coupled to the radiative transfer model. The results show a good distribution of local soil moisture within the generated SMOS pixel. Finally, the limitations of the down-scaling method are outlined.

ConclusionThe problem of distributing soil moisture within a SMOS pixel from SMOS observation at global scale and some information on the state and characteristics of the surface at local scale is not well constrained. The choice of estimating soil moisture distribution with surface temperature distribution is based on the following hypothesis: 'surface temperature varies quasi linearly with soil moisture in a given soil moisture range and in homogeneous surface conditions'. From this postulate, it is possible to formulate a local constraint function of two parameters and called the relative distribution constraint. The application of this constraint to the down-scaling problem reduces the dimension of the space of solutions from 1600 to 2. Two is also the number of independent global constraints that is possible to apply on the system: one at surface level and another at observation level. These global constraints may be used to calibrate successively both parameters of the relative distribution, the effective level parameter and the contrast parameter.The application of the down-scaling on a synthetic scene outlines the relevance of the approach. The heterogeneity of surface conditions that is likely to generate a systematic noise on distributed soil moisture is reduced and the spatial structure of generated soil moisture is well restituted. The sensitivity analysis shows a great robustness of the scheme towards uncertainties, which may be important, on local auxiliary information. However, this study shows that a limitation exists as concerned the determination of the contrast parameter when a noise is added on global observation. The multi-angular and bi-polarized capabilities of SMOS captor seem to be not sufficient for determining precisely the contrast of the relative distribution.

I. Objective of the Study

Distribution of surface soil moisture within a SMOS pixelby multi-spectral analysis

II. Formulate 3 Constraints to the Distributed System

III. Apply the Down-Scaling Scheme

Surface Variables Random Generator

Radiative Transfer

Model (L band)

SMOS global

observation

LAI

Soil T

emper

ature

Other Variables

Generate a Synthetic Scene Algorithm

Model Generated Soil Moisture

Distributed Soil Moisture

Results

IV. Limitations

Soil M

oistu

re

Olivier MERLIN*, Ghani CHEHBOUNI, Yann Kerr, Philippe RICHAUME, Pierre GENTINECESBIO, 18 Avenue Edouard Belin, Toulouse cedex 4, France

* [email protected]

Verify Primordial Hypothesis

‘Are local information

obtained in other spectral bands

(LAI, surface temperature)

sufficient to distribute Soil Moisture

given SMOS Observation?’

minimized

SMOS ObservationL band

Local information in Optic et Thermal bands

Resolution ~ 40 km

Resolution ~ 1 km

WW i

WW

WWfWW

i

iii1

SMOSBTfBT 1

211

1

fTBTBFf

WW

WWfWW

SMOS

i

iii

Relative Distribution Constraint (C1)

Surface Global Constraint (C2)

Observation Global Constraint (C3)

ii XffW 10

Distributed Soil Moisture

Level Distribution Parameter

Variable whose space variability is linked

to the space variability

of surface temperature

Contrast Distribution Parameter

‘Surface Temperature varies quasi linearly

as a function of Soil Moisture

in a specific range of Soil Moisture

and in homogeneous Surface Conditions’

Sensitivity Analysis

CaseSoil Temperature

(K)

LAI

(%)

SMOS Observation

(K)

Noise 1 2 20 0

Noise 2 4 50 0

Noise 3 0 0 1

Noise 4 0 0 2

Noise 5 0 0 4B

A W (%) f1

CaseViewing

Configuration MeanStandard

deviationMean

Standard

deviation

A 19.5 0 -3.0 0No Noise

B 19.5 0 -3.0 0

A 19.5 0.0 -3.0 0.1Noise 1

B 19.5 0.0 -3.0 0.1

A 19.3 0.1 -2.7 0.5Noise 2

B 19.3 0.1 -2.9 0.4

W (%) f1

CaseViewing

Configuration MeanStandard

deviationMean

Standard

deviation

A 19.5 0 -3.0 0No Noise

B 19.5 0 -3.0 0

A 19.5 0.3 -2.6 2.3Noise 3

B 19.5 0.1 -2.6 2.0

A 19.6 0.5 -3.0 2.5Noise 4

B 19.5 0.3 -2.9 2.2

A 19.5 1.1 -3.1 2.7Noise 5

B 19.5 0.6 -2.9 2.5

States

signed by L band

Surface

States

Measured States

C3

C2

C1

Simulated Physical States

Simulated Non-Physical States

i

imi

imSMOS XTBT ,,

i

imi

im XTBT ,,

i

im

im

i XTBT ,,

i

imSMOS XTBT ,,

i

im

im

i XTW ,, i

im

i XTW ,,

i

imi

im

i XTW ,,

i

imi

im XTW ,,

G

GP

1localRT

localRT

1globalRT

(Gglobal)

(Glocal)

(Fglobal)

(Flocal)

Radiative Transfer Layer (Model)

C1

C2

Soil moisturedistribution

Projectedsoil moisturedistribution

Dynamic increment of contrast

Contrast equal to zero (initialization)

Adjust Global level

kF Minimal value of global cost function

C3

Distributed soil moisture

(output)

Application of Filter

Surface Budget Model