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Home > Research > Ifsdocs > ASSIMILATION >  
   

DATA ASSIMILATION

IFS documentation Front Page


Table of contents

CHAPTER 1 Incremental formulation of 3D/4D variational assimilation-an overview

CHAPTER 2 3D variational assimilation

CHAPTER 3 4D variational assimilation

CHAPTER 4 Background term

CHAPTER 5 Conventional observational constraints

CHAPTER 6 Satellite observational constraints

CHAPTER 7 Background, analysis and forecast errors

CHAPTER 8 Gravity-wave control

CHAPTER 9 Data partitioning (OBSORT)

CHAPTER 10 Observation screening

CHAPTER 11 Analysis of snow

CHAPTER 12 Land surface analysis

CHAPTER 13 SST and sea-ice analysis

CHAPTER 14 Reduced-rank Kalman filter

REFERENCES

 
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12.3 Soil analysis




The soil analysis scheme is based on an "local" optimum interpolation technique as described in Mahfouf (1991) and Douville et al. (2001). The analysis increments from the screen-level analysis are used to produce increments for the water content in the first three soil layers (correponding to the root zone) :

 
(12.8)


and for the first soil temperature layer :

 
(12.9)


The coefficients and are defined as the product of optimum coefficients and minimising the variance of analysis error and of empirical functions , and reducing the size of the optimum coefficients when the coupling between the soil and the lower boundary layer is weak.

 
(12.10)


and

 
(12.11)





with

 
(12.12)


where represents the correlation of background errors between parameters and .


The statistics of background errors have been obtained from a series of Monte-Carlo experiments with a single-column version of the atmospheric model where initial conditions for soil moisture have been perturbed randomly. They were obtained for a clear-sky situation with strong solar insolation. Empirical functions are aimed to reduce soil increments when atmospheric forecast errors contain less information about soil moisture. To obtain negligible soil-moisture corrections during the night and in winter, is a function of the cosine of the mean solar zenith angle , averaged over the 6 h prior to the analysis time :

 
(12.13)


The optimum coefficients are also reduced when the radiative forcing at the surface is weak (cloudy or rainy situtations). For this purpose, the atmospheric transmittance is computed from the mean downward surface solar radiation forecasted during the previous 6 hours as :

 
(12.14)


where is the solar constant.


The empirical function is expressed as :

 
(12.15)


with and .


The empirical function reduces soil moisture increments over mountainous areas :

 
(12.16)


where is the model orography, =500 m and =3000 m.


Furthermore, soil moisture increments are set to zero if one of the following conditions is fufilled:
1)   The last 6 h precipitation exceeds 0.6 mm
2)   The instantaneous wind speed exceeds 10 m s-1
3)   The air temperature is below freezing
4)   There is snow on the ground


To reduce soil moisture increments over bare soil surfaces, the standard deviations and the correlations coefficients are also weighted by the vegetation fraction , where low and high vegetation cover are defined in Chapter 7 of the Physics Documentation.


The statistics of forecast errors necessary to compute the optimum coefficients are given in Table 12.1.


The correlations have been produced from the Monte-Carlo experiments. The standard deviation of background error for soil moisture is set to 0.01 m3m-3 on the basis of ECMWF forecasts differences between day 1 and day 2 of the net surface water budget (precipitation minus evaporation minus runoff).


The standard deviation of analysis error is given by the screen-level analysis from :

 
(12.17)


From the values chosen for the screen-level analyis and %.


Soil moisture increments are such that they keep soil moisture within the wilting point and the field capacity values, i.e. :
  •   if then
  •   if then


Finally the coefficients providing the analysis increments are :

 
(12.18)


and

 
(12.19)


The coefficient is such that soil temperature is more effective during night and in winter, when the temperature errors are less likely to be related to soil moisture. This way, 2 m temperature errors are not used to correct soil moisture and soil temperature at the same time.
Table 12.1 Statistics of background errors for soil moisture derived from Monte-Carlo experiments
Coefficient
Value

-0.82

-0.92

-0.90

0.83

0.93

0.91

1.25 K

9.5 %

-0.99



In the 12 h 4D-Var configuration, the soil analysis is performed twice during the assimilation window and the sum of the increments is added to the background values at analysis time.


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