id model takes soil and
strongest driver of the
ids and occurrences of
nations' have therefore
reflectances are shown
decrease in the visible
:getation result in high
t except Zj , £2 and cl
ad of 3200 °Q roughly
eriod. These errors are
allocation coefficient a
t is displayed on figure
ref) and the first guess
Fig. 3 Seasonal profile of reflectances. Open circles are the synthetic weekly 'observations' computed with the
LAI time profile from the reference simulation. The visible reflectance ranges from 0.18 (bare soil) to 0.044 at
maximum canopy development. The near infrared ranges from 024 (bare soil) to 0J7. The solid line
represents daily reflectances obtained with the first guess parameters.
3J.2. Assimilation of ’clean’ data. The cost function J(u), which is minimized to find the best agreement
between model and observations, was computed as follows:
7(11,£2,a) = X [(pr"-PS“) 1 +(p^T’-PS") 1 ] (2)
i-1.52 L
where p““ 1 is the visible reflectance of week i computed from the vegetation model with current Zj Z2
is the corresponding near infra-red reflectance; and p£* are the 'observed' reflectances obtained for
week i with the reference simulation. This cost function exhibits discontinuities and local plateaux in response
to Zj or Z2 variations. For this reason, we chose the downhill simplex method (Matlab, from The Math Works,
Inc.) to minimize it. This algorithm allows a very good retrieval of the parameters (table 1) when clean
observations are assimilated in die model.
GPP
NPP
1010
625
740
392
1011
625
Z1 (°Q
Z2(°Q
a
ref
600
3200
0.480
1st guess
1000
3700
0.45
retrieval
602.9
3201.9
0.479
’ and NPP values drop
¡0 respectively, mainly
Tadiance are depleted.
>00 Od too w
ce simulation. Positive
the dominant process,
?n. bottom) Difference
y develops earlier and
wading to high positive
photosynthetic rate is
Table 1 : reference parameters (ref) and retrieved parameters after assimilation of 'clean observations'. GPP
and NPP values are in g C m-2 year-1
These parameters result in the same LAI profile as the reference one. Bearing in mind the strong assumption of
a 'perfect model', one can notice that reflectances for the periods when LAI is lower than 3 allow the restitution
of the complete profile of LAI, when model knowledge is taken into account. In this perspective, it is
particularly interesting to study the stability of the assimilation scheme.
3.3.3. Assimilation of noisy 'observations'. As a step towards real data, we investigate the behavior of the
assimilation scheme when a gaussian noise is added to each synthetic observations. The objective is to asses
the quality of the retrieved parameters and the consequences on the carbon fluxes. The assumption of a perfect
model still holds, but this simulates perturbations of the satellite measurements. The noise has a zero mean and
a standard deviation of 0.02. This value corresponds to 16% of the mean visible reflectance and 5% of the
mean near infrared reflectance. The results of 50 minimizations are displayed in table 2.
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