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www.sciencemag.org/cgi/content/full/science.1184984/DC1
Supporting Online Material for
Terrestrial Gross Carbon Dioxide Uptake: Global Distribution and Covariation with Climate
Christian Beer,* Markus Reichstein, Enrico Tomelleri, Philippe Ciais, Martin Jung,
Nuno Carvalhais, Christian Rödenbeck, M. Altaf Arain, Dennis Baldocchi, Gordon B. Bonan, Alberte Bondeau, Alessandro Cescatti, Gitta Lasslop,
Anders Lindroth, Mark Lomas, Sebastiaan Luyssaert, Hank Margolis, Keith W. Oleson, Olivier Roupsard, Elmar Veenendaal, Nicolas Viovy, Christopher Williams,
F. Ian Woodward, Dario Papale
*To whom correspondence should be addressed. E-mail: [email protected]
Published 5 July 2010 on Science Express DOI: 10.1126/science.1184984
This PDF file includes:
Materials and Methods SOM Text Figs. S1 to S34 Tables S1 to S9 References
Gross Primary Production Estimation at Ecosystem Level
Estimates of GPP at the ecosystem level are based on the eddy covariance technique, the only
method that allows the direct observation of the CO2 flux between land surface and atmosphere
in a nondestructive continuous way, which has been deployed on more than 400 sites world-
wide now. The eddy covariance technique is based on high-frequency vertical wind vector and
CO2 and H2O concentration measurements using 3-D anemometer and Infraed Gas analyzers
installed at platforms well above the vegetation canopy (1,2). Half-hourly flux and meteorolog-
ical data from regional networks and individual sites were combined to create the FLUXNET
database for a workshop in La Thuile, Italy in 2007. Hence, data from the first measurement
years (e.g. 1993 in the US, 1996 in Europe) up to 2006 are included. The submission of site
data to the data base by networks or individual site investigators occurred on a voluntary basis,
i.e. the data set is a subset of all observations carried out globally. The networks Ameriflux,
CarboEurope and Fluxnet-Canada submitted their complete data sets. This resulted in a global
data set with 968 years of data from the 253 sites, with all major climate zones being represented
(although temperate climates being over-represented). After harmonization of variable names
and units as well as logical checks for obvious data errors (e.g. constant variables, impossible
values) each site-year was processed according to the methods in Reichstein et al. (3) and Papale
et al. (4), including storage correction, quality control, gap-filling and flux-partitioning. Uncer-
tainties in temporal integrals of GPP stem from uncertainties in the measurements themselves,
gap-filling procedures, and the algorithm to partition the observed net flux into GPP and ecosys-
tem respiration as discussed and analyzed in refs. (4–6). Usually the largest uncertainties in the
eddy covariance flux data are introduced by a potential so called selective systematic error (7),
i.e. an underestimation of fluxes during periods without sufficient turbulent exchange between
ecosystems and the atmosphere. This primarily occurs during night, and the friction velocity
4
(u*) which is an indirect measure of the turbulent exchange can be used as an indicator for these
situations. Thus, data below a site specific threshold of u* is being filtered out. However, this
u*-based filtering is a semi-empirical approach and subject to uncertainties itself. Hence, we
followed two ways to address this uncertainty: 1) Via a bootstrap approach, for each site year
a distribution of u*-thresholds is generated, and propagated into a distribution of GPP, after
gap-filling and flux-partitioning (4). 2) The GPP is estimated both, via a light response curve
approach using only day-time data (8) and the conventional night-time data based approach (3).
Similar to Lasslop et al. (8) differences can be large for individual sites but remain in most cases
below 70 gC/m2/a and are distributed symmetrically around zero, i.e. there is no systematic dif-
ference between night-time and day-time based GPP estimates after u*-filtering (Fig. 1). The
propagation of the uncertainties of the GPP estimates at site level into global GPP estimates has
been tested with the Model Tree Ensemble approach which has been trained separately with
day-time and night-time based estimates (see below).
Diagnostic modeling
The flux tower sites are classified by the IGBP land cover types. For each of these types, we
generally estimate parameters at daily to monthly time scales of a model M that explains GPP
by a set of environmental conditions x, M : x → GPP where x can contain the fraction of
absorbed photosynthetically active radiation (fAPAR) or climate variables, such as short-wave
radiation, air temperature, precipitation, or vapor pressure deficit, depending on the respective
model. M can be represented by the arithmetic mean (KGB), a single regression equation (MI-
AMI) or by a set of linear, non-linear or piece-wise linear equations (ANN, MTE) as explained
in more detail below. The so calibrated model is then run by global grids of the predictor vari-
ables with underlying global land cover maps. The WUE approach differs from this scheme.
With this approach, WUE instead of GPP is scaled from flux towers sites to the globe and then
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Difference between day-time and night
-time based GPP [gC m
-2yr
-1]
0.00
Difference between day time and night time based GPP [gC m yr ]
Figure 1: Distribution of differences in GPP estimations by NEE partitioning methods (3, 8) atflux tower sites.
GPP calculated by using the water balance of catchment basins[m1].
Ensemble Building and Overall Uncertainty Estimation
For each land cover type a parameter distribution is derived by randomly resampling a subset of
the set of flux tower sites (except MTE approach). This distribution accounts for uncertainties
of the site level GPP estimates and the overall sampling uncertainty. In addition, we take into
consideration potential biases in the predictor variables used for the globally distributed calcu-
lations by applying n independent predictor datasets. In conjunction with the additional usage
of m different models such scheme potentially results in n · m of the above mentioned GPP
distributions.
However, instead of full factorial model runs, we concentrate on the most sensitive drivers
6
for each approach (see detailed approach description below). For instance, the LUE approach is
a linear regression of GPP against fAPAR*PAR. Therefore, this method is sensitive to fAPAR
and radiation inputs; the extrapolation of WUE directly depends on the maximum LAI; the
KGB approach is a look-up table for ecoregions, hence sensitive to the underlying land cover
map; etc. This is detailed individually for each approach.
The parameter distribution leads to a GPP distribution for each driving dataset applied to
each model (see detailed approach description below). Then the overall GPP distribution for
each approach, and the overall GPP distribution (Fig. 1(a)) is achieved by a superimposition of
vectors with equal length representing these GPP distributions. A robust measure of standard
deviation (i.e. the median absolute deviation times 1.48) and the 95% confidence interval inform
then about the overall uncertainty taking into account uncertainty in the GPP estimation at the
flux tower sites, the globally available predictor variables, and the diagnostic model.
Representativeness of FLUXNET Sites
The eddy covariance sites are by far not homogeneously distributed over the globe, resulting
in a potential lack of representativeness. We cannot exclude that this an unknown source of
uncertainty, but there are three lines of evidence, which indicate that that the issue is not as big
as it might appear from the geographical distribution.
• The sites do represent the climate-vegetation space quite well (Fig. 2). Nevertheless no-
table gaps exist in the semi-arid-tropical areas, e.g. savannah type ecosystems. Also at
the very cold end of the climate space site are missing, but this is to a large extent very
unproductive land (including inland ice).
• An earlier study based on climate and geoecological variables similarly indicated that the
ecological representativeness of the FLUXNET sites is much better than the geographical
7
(9).
• A study with artificial data from a biosphere model indicated that the missing geographi-
cal representativeness did not hamper the retrieval of the spatial pattern of GPP using the
MTE approach (10).
These indications lend confidence that our GPP estimates are not compromised by the un-
equal spatial sampling of sites by FLUXNET from the global terrestrial surface.
Figure 2: Used flux tower sites within the temperature-precipitation space (annual basis).
Up-scaling Approaches
We have exploited almost all known approaches of how to utilize relationships between GPP and
climate and vegetation indices at site level for estimating global maps and the terrestrial total.
The GPP distributions from the individual approaches presented in the following are useful
8
to understand the uncertainty due to a single driving dataset or due to the model parameter
uncertainty for a particular approach.
Model Tree Ensemble (MTE)
The model tree ensemble approach (10) is a machine learning algorithm where the target vari-
able (GPP) is predicted by a set of multiple linear regressions from explanatory variables. Each
regression model is only valid within certain conditions defined by a hierarchical stratification
(the model tree). We established four MTEs using monthly data for: (1) predicting GPP based
on nighttime NEE data (3) and without using climate data in the regressions, (2) predicting GPP
based on daytime NEE data (8) and without using climate data in the regressions, (3) predicting
GPP based on nighttime NEE data (3) using also climate data in the regressions, (4) predict-
ing GPP based on daytime NEE data (8) using also climate data in the regressions. Type (1)
and (2) are motivated by Jung et al (11) suggesting that GPP can be predicted from remotely
sensed fAPAR alone. Training for different flux partitioning methods was used for uncertainty
analysis. A quality control filtering of the monthly FLUXNET GPP data was carried out. The
following criteria were used to remove unreliable monthly data: (1) less than 20% of mea-
sured NEE and explanatory meteorological variables were subject to uncertain gap filling, (2)
removing the 5% most uncertain data due to the uncertainty of setting the u* threshold (4), (3)
removing outliers of the difference between flux estimates from two different flux partitioning
(Reichstein, Lasslop). Regarding point (3), a non-parametric outlier test was used (median ±1.5 times interquartile range) and applied for GPP, TER, and NEE.
For each ensemble, 2500 different model trees were generated of which 25 of the best inde-
pendent trees were selected as ensemble members. In total 29 explanatory variables of four gen-
eral types were used to train MTE for predicting GPP globally: (1) monthly SeaWiFS fAPAR,
the product of fAPAR and potential radiation, and precipitation and temperature (measured at
9
the sites), (2) annual characteristics of the fAPAR seasonal cycle that describe properties of veg-
etation structure such as minimum, maximum, mean, and amplitude, (3) characteristics of the
mean annual climate such as mean annual temperature, precipitation, sunshine hours, relative
humidity, potential evapotranspiration, climatic water balance, as well as their mean seasonal
cycles derived from a global database, and (4) the vegetation type according to the IGBP classi-
fication plus a flag regarding the photosynthetic pathway (C3, C4, C3/C4) (in-situ information).
Please note that only variables of type (1) are used in the multiple linear regressions; all re-
maining variables are only used for data stratification. Spatial runs are based on gap-filled
SeaWiFS fAPAR, a land cover map (12) reclassified into the respective IGBP classes used to
describe the vegetation at FLUXNET sites from in-situ information. We generate fractions of
each class globally at 0.5◦ resolution. Grasslands are further separated into C3, C4, and mixed
C3/C4 types using the results of Winslow et al. (13); fractions of C3 and C4 crop types are
estimated using a gridded database based on FAO crop statistics (14). Various long-term mean
climatic characteristics are from CRU and correspond to the period 1961-1990. Global grids of
monthly precipitation is from GPCC; while global grids of monthly temperature is taken from
CRU-PIK. Additional runs with different temperature and precipitation data were performed
for uncertainty analysis: temperature and precipitation from CRU-PIK, and temperature and
precipitation from ERA-Interim. For these additional runs, the site-level estimation of GPP by
nighttime NEE data (3) was used.
The set-up of various MTE applications allows for analyzing the uncertainty related to: (1)
different methods of partitioning NEE measurements into GPP and TER at flux tower sites, (2)
impact of different temperature and precipitation drivers, (3) the necessity of using meteorolog-
ical variables as regressors for GPP, (4) up-scaling from FLUXNET sites, because substantial
divergence of GPP estimates within one particular ensemble essentially means that GPP rela-
tionships are not well constrained. Hence, divergence of model trees of one ensemble can be
10
interpreted as a degree of extrapolation (10).
Variables that are only split variables are only used for data stratification and do not enter
regressions. Please note that not all variables are automatically selected by the model trees.
The ’type of variability’ refers to if and when the values of the respective variable change for
a given pixel. ’Static’ variables never change and can be used by MTE to stratify into spatial
domains (e.g. according to long term mean annual temperature). ’Monthly but static over years’
refers to mean seasonal cycles, i.e. the values change monthly but the same monthly values are
repeatedly used for all years. ’Yearly’ variables have the same value within a year but this value
is updated for each year, which is primarily used for variables describing vegetation structure to
capture possible effects of land cover change. ’Monthly’ variables exhibit different values for
each month and year, i.e. they are continuously updated each for month.
11
Table 1: List of explanatory variables used for the training of the model tree ensemblesVariable Type Type of variability
Climate Mean annual temperature Split static
Mean Annual precipitation sum Split static
Mean annual climatic water balance Split static
Mean annual Potential evaporation Split static
Mean annual sunshine hours Split static
Mean annual number of wet days Split static
Mean annual relative humidity Split static
Mean monthly temperature Split Monthly but static over years
Mean monthly precipitation sum Split Monthly but static over years
Mean monthly climatic water balance Split Monthly but static over years
Mean monthly Potential evaporation Split Monthly but static over years
Mean monthly sunshine hours Split Monthly but static over years
Mean monthly number of wet days Split Monthly but static over years
Mean monthly relative humidity Split Monthly but static over years
Vegetation structure Maximum fAPAR of year Split yearly
Minimum fAPAR of year Split yearly
Maximum Minimum fAPAR Split yearly
Mean annual fAPAR Split yearly
sum of fAPAR over the growing season Split yearly
Mean fAPAR of the growing season Split yearly
Growing season length derived from fA-PAR
Split yearly
Sum of fAPAR potential radiation of year Split yearly
Maximum of fAPAR potential radiationof year
Split & regression yearly
IGBP vegetation type Split static
Meteorology Temperature Split & regression monthly
Precipitation Split & regression monthly
Potential radiation Split & regression Monthly but static over years
Vegetation status fAPAR Split & regression monthly
fAPAR x Potential Radiation Split & regression monthly
12
105
110
115
120
125
130
135
MT
E11
MT
E12
MT
E21
MT
E22
MT
E23
MT
E24
Ter
rest
rial G
PP
[PgC
/a]
Figure 3: Detailed distributions of global GPP [Pg C a−1] separately by combinations of the pre-dictor datasets. Shown are the median, 25 and 75 percentiles, and the 95% confidence interval.
• MTE11: no climate data, just SeaWifS fAPAR, daytime-based GPP; 1998-2005
• MTE12: no climate data, just SeaWifS fAPAR, nighttime-based GPP; 1998-2005
• MTE21: daytime based GPP, CRU temp plus GPCC precip, SeaWifS fAPAR; 1998-2005
• MTE22: night-time based GPP, CRU temp + GPCC precip, SeaWifS fAPAR; 1998-2005
• MTE23: night-time based GPP, pure CRU, SeaWifS fAPAR; 1998-2005
• MTE24: night-time based GPP, pure ECMWF ERA-Interim, SeaWifS fAPAR; 1998-
2005
13
Table 2: Mean and standard deviation of model performance indicators over the 25 model treesof the ensemble. All measures are based on 10-fold cross-validations performed in the leavesof the model trees. Different number of site months used for versions including or excludingmeteorological data is due to data availability of measured meteorology at the sites.
MTE type 1 MTE type 2 MTE type 3 MTE type 4R2 0.847 [0.006] 0.845 [0.007] 0.859 [0.005] 0.856 [0.006]RMSE 1.134 [0.0237] 1.14 [0.027] 1.109 [0.019] 1.117 [0.023]N parameters 107.68 [14.92] 106.84 [15.54] 122.44 [11.9] 118.4 [12.77]Adj R2 0.843 [0.006] 0.841 [0.007] 0.854 [0.005] 0.852 [0.006]N 4209 4209 3800 3800
14
Artificial Neural Network (ANN)
The ANNs are purely empirical non-linear regression models consisting of nodes connected
by weights which effectively are the regression parameters. The ANNs used are feed-forward
backpropagation networks and the weights values are adjusted during the training phase by
back-propagating the error in the prediction of the output. The training is based on a dataset of
measured examples composed by the predicting variables and the output to estimate.
Training datasets have been composed by daily eddy covariance data; input variables used
have been (1) mean air temperature (Tair), (2) daytime VPD (VPD), (3) incoming radiation
(Rg), (4) FAPAR and (5-6) top of atmosphere incoming radiation (ToAR) and first derivative of
(ToAR) as signal for the seasonality (15) while the output value has been GPP derived using the
method described in Reichstein et al. (3). Daily measured data have been filtered by removing
daily values where GPP or one of the input was calculated using less than 75% of original data
or high quality gap-filled data (see ref. (3)).
Ten different ANNs have been trained for each combination between Plant Functional Types
based on the SYNMAP classification and Climatic regions according with the KG classifica-
tion. In total 14 PFT classes (ENF, EBF, DBF, MF, CSH, OSH, WSA, SAV, GRAC3, CROC3,
WSAC4, GRAC3C4, GRAC4 and CROC4; see (16) for abbreviations and C3, C4 refers to pho-
tosynthetic pathways) and 7 climatic classes (Tropical, Dry, Subtropical/Mediterranean, Tem-
perate, Temperate Continental, Boreal and Arctic) have been used.
To train each of the 10 ANNs for each PFT-Climate combination a subset of the training
dataset (75%) has been randomly extracted and 8 ANNs with different structure (different num-
ber of nodes in the hidden layer/layers) have been trained 30 times each one, starting from
different initial weights. In total 240 (8x30) ANNs have been trained for each extraction and
for each PFT-Climate combination and the one with best performance in predicting the 25%
of data not used in the training and the simplest structure (less parameters) has been selected,
15
resulting in 10 ANNs for each PFT-Climate class (one for each extraction).
The 10 ANNs selected has been applied to the pixels where the relative PFT-Climate com-
binations were present, using two different gridded datasets:
• ANN1: Tair, VPD and Rg from ERAInterim reanalysis and fAPAR from SeaWifs (years
1998-2005)
• ANN2: Tair, VPD and Rg from GMAO GEOS400 reanalysis and fAPAR from SeaWifs
(years 2000-2005)
Using this set-up of the training it has been possible to include uncertainty estimation due to
differences in the training dataset (through the 10 extractions), differences in the model structure
(through the different ANN setups) and differences in the gridded driving variables.
Since the ANNs were trained by local meteorological variables measured at the sites, the ap-
plication of multiple climate reanalysis datasets provides highest uncertainty ranges. In contrast,
the uncertainty estimation due to different fAPAR grids should be small (cf. also LUE approach)
because the ANNs were trained by the cutouts of these grids. However, even this new applica-
tion of GMAO reanalysis climate data results in a low 2 Pg C a−1difference of the median GPP,
and the 95% confidence interval increased only slightly from 8 to 10 Pg C a−1(Fig. 4).
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125
126
127
128
129
130
131
132
133
AN
N1
AN
N2
Ter
rest
rial G
PP
[PgC
/a]
Figure 4: Detailed distributions of global GPP [Pg C a−1] separately by combinations of the pre-dictor datasets. Shown are the median, 25 and 75 percentiles, and the 95% confidence interval.
17
Light Use Efficiency (LUE)
The light use efficiency (LUE) model (17) relates GPP to the amount of absorbed photosyn-
thetically active radiation (APAR), constrained by minimum daily temperature (T) and daytime
vapor pressure deficit (VPD) (18, 19):
GPP = LUE · f(V PD) · g(T ) · APAR (1)
The model parameters were calibrated in a Bayesian framework (20) for each measurement
site in FLUXNET. This technique integrates the prior knowledge of parameter values and eddy
covariance measurements along with their associated uncertainty. This allows the estimation
of a posteriori probability distributions for model parameters (21). Prior model parameter un-
certainty was derived from the literature (19) and measurement uncertainties were assessed
according to the method developed by Lasslop et al. (22).
For the in-situ calibration, the site meteorology and remotely sensed fAPAR values corre-
sponding to the site’s geographic position were used. This calibration assumes correspondence
between the footprint of the eddy covariance station and the resolution of the fAPAR product.
The calibration results were stratified per vegetation type (PFT) and when a sufficient number
of sites were available, a simplified version of the Koeppen-Geiger climate classification were
also used (23).
Subsequently, the joint probability density functions of model parameters were randomly
resampled to apply the model spatially for the different classes. Downward shortwave radiation,
daytime vapor pressure deficit, and minimum temperature provide the meteorological forcing
of the model. Model calibration and the uncertainty propagation were performed independently
for each different fAPAR product (Fig. 5).
This analysis is accounting for flux measurement uncertainty by means of the data assim-
18
ilation technique that underpin it. Furthermore, the method allows estimating the uncertainty
related to the spatial distribution of the measurement network to be included because of the up-
scaling of model parameters done by means of stratifying the whole dataset by vegetation and
climate classes. Conversely, this does not account for specific conditions that may arise, such
as different photosynthetic pathways. As already shown by other authors (24) the use of diverse
meteorological drivers may influence the spatial patterns of the estimated GPP. Therefore, in
this study, we account for this by using forcing fields from GMAO and ECMWF. The choice of
a specific fAPAR dataset may significantly affect the model results (25) which is why we use
three independent fAPAR products based on MODIS, SeaWiFS and SPOT VGT here.
98
100
102
104
106
108
110
112
LUE
11
LUE
12
LUE
13
LUE
21
LUE
22
LUE
23
Ter
rest
rial G
PP
[PgC
/a]
Figure 5: Detailed distributions of global GPP [Pg C a−1] separately by combinations of the pre-dictor datasets. Shown are the median, 25 and 75 percentiles, and the 95% confidence interval.
• LUE11: MODIS fAPAR, ECMWF ERA-Interim; 2001-2005
• LUE12: SeaWiFS fAPAR, ECMWF ERA-Interim; 1998-2004
19
• LUE13: SPOT VGT fAPAR, ECMWF ERA-Interim; 2000-2003
• LUE21: MODIS fAPAR, DAO; 2001-2005
• LUE22: SeaWiFS fAPAR, DAO; 2000-2004
• LUE23: SPOT VGT fAPAR, DAO; 2000-2003
20
Water Use Efficiency (WUE) Approach
GPP of a whole catchment basin can be estimated by multiplying the mean water use efficiency
WUE =(
GPPET
)of the watershed with its annual water balance (ET) (26). Here, ET stands
for transpiration plus soil evaporation beneath the canopy. This concept has the fortune that a
matter flux at the regional scale (the catchment basin runoff), which integrates ecophysiological
processes at this large scale, constrains the envisaged carbon flux at the same scale. This is
a forthcoming for estimating a global number and uncertainty, but the coarse resolution limits
further spatially explicit analyzes. A further shortcoming is that not all land is covered by
watersheds for which runoff data is available.
Both, the mean WUE of the whole watershed and the ET need to be estimated. ET is
estimated by total annual precipitation of the catchment basin minus annual runoff minus annual
interception. Interception is calculated by an empirical relationship to LAI and precipitation for
each land cover type following (27). The mean WUE estimation is described below.
Water Use Efficiency Approach
At the ecosystem level, WUE can be expressed as the ratio between GPP and evapotranspiration
(ET), both of which estimated by means of the eddy covariance technique (28). For this purpose,
soil evaporation and interception need to be kept to a minimum, as they are not related to
stomatal conductance. The assumption that soil evaporation and interception are negligible after
three consecutive days without rainfall is fairly acceptable. A simple extrapolation of WUE to
the land surface made by multiplying point scale flux tower WUE estimates by the area of
each biome, however, is not valid because relationships of WUE to environmental conditions
are confounded by the effect of VPD on the water flux (29, 30) regardless of the performance
of carboxylation in relation to inner-leaf CO2 concentration. Therefore, (31) introduced the
concept of inherent WUE (IWUE) which approximates intrinsic WUE (carbon assimilation
21
divided by stomatal conductance) at the ecosystem level:
IWUE =GPP
ET· V PD. (2)
By making use of ecosystem-level measurements made by the global network of eddy co-
variance flux towers FLUXNET (31) report on a linear relationship of IWUE to both relative
soil water content at field capacity (θ) and maximum light absorption by leaves in forests:
WUEi = a · θ + b · (1− exp(−k · LAI)) , (3)
k being 0.7 for deciduous broad-leaved forests and 0.5 otherwise. This model is able to explain
over 50 % of IWUE variability in forests (RMSE=4.3 g/kg*hPa). In herbaceous ecosystems
only a relationship to LAI was found which also explains over 50 % of the IWUE variability
(31):
WUEi = b · (1− exp(−0.4 · LAI)) (4)
with b being 2 times higher for C4 ecosystems compared to C3 ones (32, 33). Both predictor
quantities can be assessed by using remotely sensed information on maximum leaf area index
(LAI) and land cover, and spatial details of the soil texture type. The combination of such
global fields with the empirical relationships found at flux tower sites enables a global mapping
of IWUE, from which a global map of mean WUE is achieved by dividing the IWUE map by
daylight VPD averaged during the growing season.
The land cover information is used to distinguish between ecosystems for application of
models described by Eq. 3 and Eq. 4. These models were derived by a holistic approach of con-
sidering ecosystems as aggregation of different plant types, such as trees and grasses, i.e. field
capacity of the soil and LAI of trees are used in the regression analysis with observed IWUE for
forests. The application of such approach, however, provoked a bias in C4-ecosystems when
there is a significant tree cover but dominant vegetation type is C4-herbaceous. The land cover
22
map indicated grassland or cropland but the remotely sensed LAI value would be much higher
than for pure herbs having a significant impact on IWUE of the catchment basin. We make use
of the MODIS Vegetation Continuous Fields product (34) for a linear mixing of Eq. 4 utilizing
C3 or C4 parameters in regions with combined occurrence of C4 grass and trees. Natural oc-
currence of C4 species (Fig. 6) is modeled by the bioclimatic zone approach following ref. (35).
An analogous linear mixing is applied for agricultural regions using the ratio of cultivated C3
and C4 species based on statistics from the FAO Statistical Yearbook 2004 (36) on a country
level (Fig. 7).
0
0.2
0.4
0.6
0.8
1
Figure 6: Climate driven occurrence of C4 herbaceous vegetation following ref. (35).
Uncertainties
GPP estimation at watershed scale by using the concept of WUE is uncertain in the following
ways:
• Uncertain remote sensing information about land cover and maximum annual LAI
• Uncertain global distribution of soil texture type
• Uncertain mean growing-season daylight VPD from climate reanalysis
23
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
Figure 7: Ratio between agricultural C3 and C4 vegetation following the FAO Statistical Year-book 2004 (36).
• Uncertain precipitation data and uncertainties in the interception loss calculation
• Uncertainty in river runoff data is neglected in this study.
• GPP is derived by flux partitioning of NEE at flux tower sites following Reichstein et
al. (3). With the WUE approach we do not address this rather small (8) uncertainty
explicitly, cf. results by the MTE1 versus MTE2 approach.
• Representativeness of flux tower sites, uncertainties in eddy covariance data processing
(cf. respective sections).
• Uncertainties in parameter estimation by the regression analysis are addressed by esti-
mating a parameter distribution instead of only one parameter value (31).
Uncertainties in remote sensing data are considered by using land cover and LAI products
both based on two different optical sensors, SPOT Vegetation (37,38) and TERRA MODIS (39,
40). These independent remote sensing products were resized to a common pixel size (1/112◦ ),
and the land cover classification harmonized to the IGBP definition. Spatial details of soil
24
texture type (41) are translated into relative soil water content at field capacity by using statistics
from Cosby et al. (42). These values are interpolated then to match the resolution of remote
sensing products. The combination of the full parameter distribution of Eq. 3 and Eq. ?? with
the different remote sensing maps led to 1372 global maps of IWUE with a spatial resolution
of 1/112◦ which is immediately averaged to 10 minutes for reasons of memory handling. For
further estimation of WUE fields we used a map of daylight VPD during the growing season
from the Global Monitoring and Assimilation Office (GMAO) GEOS400 reanalysis fields (43,
44).
The long-term precipitation of the watersheds was estimated from grids by the Climate Re-
search Unit of the University of East Anglia (CRU CL 2.0), and from the Global Precipitation
Climatology Project (GPCP, http://www.gewex.org/gpcp.html). In concert with a long-term av-
erage of river runoff that was downloaded from the Global Runoff Data Centre of the Federal In-
stitute of Hydrology (http://www.bafg.de/cln 005/GRDC/) this led to two different basin-wide
water balance values, which was then multiplied to the 1372 IWUE maps. For land that could
not be assigned to any river discharge data, potential evapotranspiration (45) is used instead of
precipitation minus runoff if the ratio of precipitation to potential evapotranspiration is higher
than 1.2 (no water limitation of GPP). This is in particular true for most of the productive land
in south-east Asia. In so doing, GPP of 84 · 106km2 land was estimated by the WUE approach.
GPP of the remaining 38 · 106km2 was filled with the median form approaches MTE1, MT2,
ANN, LUE, and KGB, in total 27 Pg C a−1.
Correction for Missing Energy Balance
For the WUE approach, another uncertainty arises from the fact that water-fluxes from eddy
covariance are used: with higher water fluxes, one gets proportionally lower WUE estimates and
consequently lower calculated GPP at catchment scale. It is a known issue, that the observed
25
0.78 0.8 0.82 0.84 0.860
10
20
30
40
50
Correction factor
Fre
quen
cy
Figure 8: Distribution of FLUXNET correction factors for evapotranspiration to meet the energybalance at the site
energy balance at eddy covariance sites is not closed. This non-closure is most often related
to an underestimation of the turbulent fluxes, has been quantified to vary around 20%, but can
vary considerably between sites ( (46)). Hence for this study we calculated the energy balance
ratio (EBR, ( (46)) for each site year, and via a bootstrap approach estimated the mean EBR for
the sites and the distribution of the expected mean (Fig. 8) . With a Monte-Carlo approach we
propagated the uncertainty of the EBR into the global GPP estimates from the WUE approach
by multiplying the GPP distribution with the distribution of the EBR factors (Fig. 8).
GPP Results by the WUE Approach
Fig. 9 shows two boxplots with the GPP distributions that stem from a) model parameter distri-
butions and the two different precipitation datasets. These results show that the uncertainty of
land cover and maximum LAI on the global GPP number is as high as the uncertainty of model
parameters and precipitation. Further investigations need to clarify if there is a high or low bias
in the MODIS or SPOT VGT based maximum LAI values, respectively.
• WUE1: MODIS based land cover and LAI; long-term average
26
118
120
122
124
126
128
130
132
134
WU
E1
WU
E2
Ter
rest
rial G
PP
[PgC
/a]
Figure 9: Detailed distributions of global GPP [Pg C a−1] separately by combinations of the pre-dictor datasets. Shown are the median, 25 and 75 percentiles, and the 95% confidence interval.
• WUE2: SPOT VGT based land cover and LAI; long-term average
27
Longitude [deg]
La
titu
de
[d
eg
]
−180 −150 −120 −90 −60 −30 0 30 60 90 120 150 180−90
−60
−30
0
30
60
90
none
Trop.
Arid
T.Dry.
T.Hum.
Sn.Warm
Sn.Cold
Polar
Figure 10: Simplified Koeppen-Geiger map
Koppen-Geiger cross Biome (KGB)
The KGB is a look-up table approach that incorporates mean annual GPP estimates for different
climate classes, given by a simplified version of the Koeppen-Geiger classification (KG map
(23)), and for different biome types (B), based on local land cover classifications. The site level
estimates of GPP stem from the flux-partitioning method described in ref. (3). When a certain
KGxB combination is not present in the set of eddy-covariance sites used, such entry in the
look-up table is given by the mean of the respective KG class for all biomes. The resulting
look-up table is up-scaled making use of the global Koeppen-Geiger classification map Fig. 10
and land cover classification maps: 1) SYNMAP (12), 2) GLC2000 (37), and 3) MODIS (39).
The uncertainties from the KGB approach stem from: a) the u* threshold used for NEE ”u*-
correction”; b) the partitioning of NEE into GPP and TER (3); c) the filling of empty KGxB
combinations; d) the land cover datasets used to propagate GPP globally; e) the climate datasets
used for the Koeppen-Geiger classification. The uncertainty characterization focuses: a) the de-
termination of the u* threshold, by following a bootstrap approach, with 500 resamplings (47),
to estimate the distribution of the mean annual GPP per KGxPFT combination; b) the changes
in global GPP estimates driven by different land cover classification maps: 1) SYNMAP; 2)
28
0 50 100 150
SYNMAP
MODIS
GLC2000
GPP Pg C yr−1
Land
cov
er m
ap
ENFEBFDNF+DBFMFCSHOSHWSASAVGRAWETCRO
Figure 11: Distribution of global GPP estimates per land cover class
MODIS; 3) GLC2000.
Globally, land cover is an important factor for the uncertainties in the KGB approach and the
differences in GPP between land covers is statistically significant (Fig. 11). Despite the over-
all global differences, the dissimilarities between the three land cover maps embed significant
differences in the partial contributions of each class for the global GPP estimate.
• KGB1: GLC2000 land cover; long-term average
• KGB2: MODIS land cover; long-term average
• KGB3: Synmap land cover; long-term average
29
120
122
124
126
128
130
132
134
136
138
KG
B1
KG
B2
KG
B3
Ter
rest
rial G
PP
[PgC
/a]
Figure 12: Detailed distributions of global GPP [Pg C a−1] separately by combinations of thepredictor datasets. Shown are the median, 25 and 75 percentiles, and the 95% confidence inter-val.
30
MIAMI Model
Annual net primary productivity has been related to mean annual temperature and precipitation
in the MIAMI model by Lieth (48). We adopted the MIAMI model for GPP and normalized it
to reference conditions, i.e. a mean annual temperature of 15 ◦C and precipitation of 1000mm:
GPP = min [g (MAT ) , f (P )] , (5)
with
g (MAT ) = GPP15degC · 1 + ea1−a2·15degC
1 + ea1−a2·MAT(6)
f (P ) = GPP1000mm · 1− e−k·P
1− e−k·1000mm(7)
where MAT is mean annual temperature [ ◦C ], P is the annual precipitation and the other
variables are parameters to be estimated. We re-parameterized this model with the mean annual
GPP, mean annual temperature and precipitation estimates at the eddy covariance flux tower
sites. Annual data was only used when there was more than 85% of reliably filled (see ref. (3))
flux and meteorological data and the longest data gap within a year was shorter than 20 days.
When several years of data were available those were aggregated into one average, in order to
avoid giving too much weight to sites with multiple years. The parameterized model was then
applied globally on a grid with 0.5◦ latitudinal and longitudinal resolution by utilizing available
data sets for temperature and precipitation. The GPP of non-vegetated area has been set to zero,
but no effect of vegetation structure or species-specific function is taken into account. Uncer-
tainties within this approach may arise from uncertainties in a) the parameter estimation, b) the
eddy covariance flux data, particularly the partitioning of the net flux into GPP and ecosystem
respiration, and c) the meteorological data sets used to apply the parameterized model globally.
31
The parameter estimation uncertainty was addressed via a bootstrap approach (?, 47), with 500
resamplings of all 138 sites.
Uncertainties in the partitioning of the eddy covariance data stem from the eddy covariance
data itself (in particular during night-time) and from uncertain model assumptions underlying
the partitioning of the net CO2flux into GPP and ecosystem respiration. We addressed this by
using two fundamentally different flux-partitioning algorithms: One algorithm is using night-
time data to parameterize ecosystem respiration as function of temperature and time-varying
base respiration, which is then extrapolated into the day (3). The other is using day-time data
to parameterize a response function of NEE to incoming short wave radiation, air temperature
and vapor pressure deficit of the air (8). We parameterized the MIAMI model with the GPP es-
timates from both algorithms and did not find significant differences in the parameter estimates.
The model explained 71% of the variance in GPP, with the parameters depicted in Tab. 3. GPP
residuals still show a clear association with fAPAR (Fig. 14) demonstrating the importance of
remotely sensed information about vegetation function and structure. Global meteorological
data sets are much more uncertain with respect to precipitation, compared to temperature (24).
Hence we concentrated the uncertainty analysis on the effect of precipitation by using six differ-
ent sources: CRU CL 2.0, CRU TS 2.1, CMAP, DELAWARE, GPCP, ECMWF, ERA-interim.
Furthermore, CRU TS 2.1 temperature forcing was used. Figure 13 shows the effect of the
different precipitation data sets on the estimation of global GPP, as well as the model parameter
uncertainty, given a precipitation data set.
• MIAMI1: CRU temp, CRU CL 2.0 precip; long-term average
• MIAMI2: CRU temp, CRU TS 2.1 precip; 1998-2002
• MIAMI3: CRU temp, CMAP precip;
• MIAMI4: CRU temp, DELAWARE precip; 1998-2005
32
Table 3: Parameterization of the MIAMI modelParameter Estimate (±1SE)GPP15 1923 (128) gC m-2 yr-1GPP1000 1827 (63) gC m-2 yr-1a1 242 (2.89)a2 0.049 (0.0038) ◦C -1k -0.00025 (0.00019) mm-1
135
140
145
150
155
160
MIA
MI1
MIA
MI2
MIA
MI3
MIA
MI4
MIA
MI5
MIA
MI6
Ter
rest
rial G
PP
[PgC
/a]
Figure 13: Detailed distributions of global GPP [Pg C a−1] separately by combinations of thepredictor datasets. Shown are the median, 25 and 75 percentiles, and the 95% confidence inter-val.
• MIAMI5: CRU temp, GPCP precip; 1998-2005
• MIAMI6: CRU temp, ECMWF ERA-Interim precip;
33
Figure 14: Relationship of the residual GPP from the parameterized MIAMI model (observedminus modeled) with mean annual fAPAR from SEAWIFS. For visual clarity the fAPAR datahas been aggregated into 12 percentile classes, each of them represented by the circle and errorsbars as mean and +-1 standard error. Regression line, 95% confidence bands and the regressionstatistics are shown as well.
34
Summary Predictor Datasets Usage for Up-scaling Approaches
Table 4: Driving data for the six diagnostic models
Approach fAPAR rad. temp. precip. vapor runoff land spatial temporal
or LAI pressure cover resolution resolution
deficit
MTE1 X X X X - - X 0.5◦ monthly
MTE2 X - X X - - X 0.5◦ monthly
ANN X X X X X - X 0.5◦ daily
WUE X - - X X X X 1km to water-shed
long-term
KGB - - X X - - X 1km to 0.5◦ monthly
MIAMI - - X X - - - 0.5◦ monthly
35
Figure 15: Regression between GPP and ∆NEE based on measured NEE and derived GPP atflux tower sites. Shown is the example for the 30◦ latitudinal band around 55◦ N.
NEE Amplitude Approach
First, a linear relation between annual GPP and the seasonal NEE amplitude is determined
from flux tower sites for 30◦ -wide latitudinal moving bands (Fig. 15). Second, this linear
regression model is applied to the seasonal NEE amplitude derived from atmospheric CO2 con-
centrations and an inversion of their atmospheric transport (update of (49), Jena inversion,
s 99v3.1 monthly.nc).
36
−150 −100 −50 0 50 100 150
−80
−60
−40
−20
0
20
40
60
80
0
200
400
600
800
1000
1200
1400
1600
(a)
−150 −100 −50 0 50 100 150
−80
−60
−40
−20
0
20
40
60
80
0
500
1000
1500
2000
2500
3000
3500
(b)
Figure 16: 16(a), 16(b) Spatial details of annual GPP [gC/m2/a] in extra-tropical regions basedon an independent scaling from flux tower sites to the region based on the relationship of annualGPP to the seasonal amplitude of NEE.
37
Summary of Data used
Here we briefly summarize and cite the data and data products used from site-level to global.
At flux tower stations measurements of net ecosystem exchange (NEE) were taken to estimate
gross primary production (GPP) as described in refs. (3, 8). At these sites, meteorological
information in addition to NEE was available with 30-minutes temporal resolution. For the
application of the diagnostic models, we mainly used the fraction of absorbed photosyntheti-
cally active radiation (fAPAR) based on SeaWiFS (50), but for the LUE approach also based
on MODIS (40) and SPOT VGT (38). The land cover maps are SYNMAP (12) based on the
sensors AHVRR, MODIS, and SPOT Vegetation, and in addition GLC2000 (SPOT Vegetation),
MOD12 (39), and MODIS VCF (34). Two LAI datasets have been used, from the CYCLOPES
project based on SPOT Vegetation (38), and based on the MODIS sensor (40). Finally, climate
fields from ECMWF ERA-Iterim (51), GMAO GEOS400 (44, 52), CRU TS 2.1 (53), and CRU
CL 2.0 (54), as well as precipitation from the GEWEX project Global Precipitation Climatology
Project (GPCP, http://www.gewex.org/gpcp.html), the GPCC Global Precipitation Climatology
Centre (55), and Delaware (GHCN) (56) have been applied. We have used river runoff data
that was downloaded from the Global Runoff Data Centre of the Federal Institute of Hydrology
(http://www.bafg.de/cln 005/GRDC/).
38
Process-based biosphere models and modeling protocol
The models ORganizing Carbon and Hydrology in Dynamic EcosystEms (ORCHIDEE) (57),
and Community Land Model (CLM-CN) version 4 (58) represent key ecosystem processes gov-
erning biogeochemistry and biophysics of the land surface. Spatial heterogeneity is represented
as a nested sub-grid hierarchy in which grid cells are composed of fractions of land units, soil
and canopy columns, and up to 15 plant functional types (PFTs). Biogeophysical processes are
simulated for each sub-grid unit independently, and the surface variables and fluxes are then av-
eraged by area. In so doing, the PFT composition of each grid cell and related maximum LAI is
prescribed. The Lund-Potsdam-Jena Dynamic Global Vegetation Model (LPJ-DGVM) (59,60),
LPJmL (61) and SDGVM (62,63) additionally predict the composition of natural PFTs as a con-
sequence of competition. These models were driven with differing climate datasets. We have
chosen for each model the maximum period within 1998-2005 to calculate average annual GPP.
This is 1998-2002, 1998-2003, and 1998-2004 for SDGVM, LPJ-DGVM and CLM-CN, re-
spectively. However, aggregation tests showed no difference in the presented results in Fig. 3 of
the main paper (not shown). In contrast, aggregation experiments with the LPJ-DGVM demon-
strated that the spatial partial correlations are subject to the spatial resolution, with deviations
to the 0.5◦ results when being higher than 1.5◦ by1.5◦ (not shown). Therefore, only global
models with approximate one degree or less were included into the analysis. All climate drivers
are either observation-based from CRU or normalized to CRU. Therefore, process model results
were only correlated to CRU climate data.
LPJ-DGVM and LPJmL
The LPJ-DGVM (59, 60) was driven by monthly CRU-PIK climate fields with 0.5◦ pixel size
(53, 64). As a non-gridded global input, annual CO2 concentrations were used that were de-
rived from ice-core measurements and atmospheric observations provided by the Carbon Diox-
39
ide Information Analysis Center (http://cdiac.esd.ornl.gov/index.html). In addition, globally
available soil texture classes with 0.5◦ resolution (65) were used. The model was run until the
carbon pools reached equilibrium based on transient climate (1901-1930) and under constant
pre-industrial atmospheric CO2 concentration (280 ppm). Weather generator algorithms were
employed to disaggregate monthly climate variables into daily values.
Inputs for the LPJmL (61) runs were similar, but extended CRU-PIK climate until 2005 was
used. The modeling protocol is described in Jung et al. (10), and the establishment of the land
use data set (crop distribution, irrigated areas, etc) is described within Fader et al. (66).
CLM-CN
The Community Land Model version 4 is described by (58). The model includes a carbon-
nitrogen biogeochemistry sub-model that simulates leaf area index, stem area index, and canopy
height (CLM4CN). For these simulations, a 57-year (1948-2004) meteorological dataset was
used to force the model in offline simulations uncoupled from a climate model, as in (67). Land
cover, atmospheric CO2, and atmospheric nitrogen deposition were held constant at values for
year 2000. The spatial resolution of the model is 1.25 degrees in longitude by 0.9375 degrees
in latitude. For the correlation analyses the model results were interpolated bi-linearly to the
0.5◦ by0.5◦ resolution that is used by the data-driven approaches and the other process models.
The simulations were driven using a 57-year (1948-2004) atmospheric forcing dataset (68,
) with 3-hourly and 1.875 degree resolution. The forcing dataset is derived from the Na-
tional Centers for Environmental Prediction-National Center for Atmospheric Research (NCEP-
NCAR) reanalysis with monthly mean near-surface air temperature and precipitation from the
reanalysis corrected to observed monthly mean values; downward solar radiation adjusted for
observed cloud cover and then for mean biases; surface specific humidity adjusted using the
adjusted surface air temperature and reanalysis relative humidity; and surface wind speed and
40
air pressure taken directly from the reanalysis data.
ORCHIDEE
The forcing data of ORCHIDEE (57) was the CRUNCEP data which is describe in http://dods.extra.cea.fr/data/p529viov/cruncep/readme.htm.
Vegetation was fixed to those of year 2000 and then the vegetation was first spinup to an hy-
pothetical equilibrium in year 1860 (using climate for year 1901 to 1910 in a loop) with the
CO2 of 1860. Then the model was run for 40 years with a constant climate from 1901 to 1910
with increasing CO2 from 1860 to 1900, then followed the transient simulation from 1901 to
2008 with increasing climate and CO2.
SDGVM
The SDGVM (62, 63) was driven by monthly fields from CRU TS 2.1 (0.5◦ ,1901-2002) but
ECMWF ERA-40 reanalysis data was used for the interpolation by a weather generator. The
land cover was prescribed according to the GLC2000 land cover map (37). Initialization for
1901 was done using a 500 year spin-up composed of randomized 1901-1920 climate.
41
Biome map
Figure 17: Biomes of the world as defined by Prentice et al. (69) based on the Olson ecorgionsmap (70). The cropland area came from the MODIS land cover map (39). These biomes areused for Tab. 1 and Tab. 2 of the main paper, Tab. 5, and Tab. 6.
42
Mean GPP per biome
For each up-scaling approach, a spatially explicit GPP distribution was estimated by propagat-
ing parameter uncertainty and by using several predictor datasets, i.e. for each 0.5◦ by 0.5◦ pixel
we estimated a GPP distribution. This distribution was represented by differing number of repli-
cates for each approach, but we randomly resampled 200 out of the original number, ranging
from 25 (MTE) to 2744 (WUE). These distributions were superimposed for estimating the me-
dian and median absolute deviation times 1.48 (uncertainty) of the global number, but also of
the biome specific results.
Table 5: Mean annual GPP per area [gC/m2/a] for all biomes and for each up-scaling scheme(columns 2-8). Column 9 shows the median. Column 10 shows the biome area in 1012m2 (69).Column 11 shows the median GPP [Pg C a−1] of each biome from the individual GPP distribu-tions. The sum of these biome-wide GPP results does not meet the 123 Pg C a−1 estimated byour up-scaling (Fig. 1(a) of the main paper) because the underlying biome areas do not neces-sarily agree. Column 12 shows the comparison to the estimates by Prentice et al. (69) [Pg C a−1]by doubling NPP values from Saugier et al. (71).
Biome MTE1 MTE2 ANN LUE WUE KGB MIAMI Median Area GPP GPP=2*NPP
Tropicalforests
2256.1 2412.1 2443.5 2112.1 2332.9 2223.9 2663.4 2332.9 17.5 40.8 43.8
Temperateforests
933 954.4 928.8 895.3 1013.8 1033.9 1093 954.4 10.4 9.9 16.2
Borealforests
604.6 620.8 505.7 462.8 690.4 535.1 697.8 604.6 13.7 8.3 5.2
Tropicalsavannahs&grasslands
1053.7 1134.9 1339.1 900.4 1041.6 1225.5 1693.7 1134.9 27.6 31.3 29.8
Temperategrasslands& shrub-lands
372.1 400.7 478.2 376.4 622 664.9 736.7 478.2 17.8 8.5 14
Deserts 151.1 231.5 290.5 134.5 228.7 427.3 421.4 231.5 27.7 6.4 7
Tundra 236.7 292.9 213.6 131.6 329.6 301.6 490.2 292.9 5.6 1.6 1
Croplands 1015.8 1029.4 1094.6 935.2 1133 1134.5 1413.9 1094.6 13.5 14.8 8.2
Wetlands 980.7 1051.2 1203.8 902.1 952 1165.2 1484.6 1051.2 0 0 0
Mean/Total 844.9 903.1 944.2 761.2 927.1 968 1188.3 908.4 133.8 121.7 125.2
43
Spatial details and latitudinal means of median GPP results bythe individual up-scaling approaches
Median GPP [gC/m2/a] of approach MTE1
0
500
1000
1500
2000
2500
3000
3500
Figure 18: Spatial distribution of median GPP by the MTE1 approach
44
Median GPP [gC/m2/a] of approach MTE2
0
500
1000
1500
2000
2500
3000
3500
Figure 19: Spatial distribution of median GPP by the MTE2 approach
Median GPP [gC/m2/a] of approach ANN
0
500
1000
1500
2000
2500
3000
3500
Figure 20: Spatial distribution of median GPP by the ANN approach
45
Median GPP [gC/m2/a] of approach LUE
0
500
1000
1500
2000
2500
3000
3500
Figure 21: Spatial distribution of median GPP by the LUE approach
Median GPP [gC/m2/a] of approach WUE
0
500
1000
1500
2000
2500
3000
3500
Figure 22: Spatial distribution of median GPP by the WUE approach
46
Median GPP [gC/m2/a] of approach KGB
0
500
1000
1500
2000
2500
3000
3500
Figure 23: Spatial distribution of median GPP by the KGB approach
Median GPP [gC/m2/a] of approach MIAMI
0
500
1000
1500
2000
2500
3000
3500
Figure 24: Spatial distribution of median GPP by the MIAMI approach
47
−50 −25 0 25 50 750
500
1000
1500
2000
2500
3000
3500
4000
4500
5000
Latitude [°]
GP
P [g
C/m
2 /a]
Data−drivenProcess models∆ NEE
Figure 25: Data-driven and process-based ranges and medians of latitudinal GPP means.
−50 −25 0 25 50 750
500
1000
1500
2000
2500
3000
3500
4000
4500
5000
Latitude [°]
GP
P [g
C/m
2 /a]
Data−driven rangeLPJLPJmLORCHIDEECLM−CNSDGVM∆ NEE
Figure 26: Data-driven ranges and individual process-based resullts of latitudinal GPP means.
48
−50 −25 0 25 50 750
500
1000
1500
2000
2500
3000
Latitude [°]
GP
P [g
C/m
2 /a]
RangeMTE1MTE2ANNLUEKGB∆ NEE
Figure 27: Data-driven ranges and individual results of latitudinal GPP means.
49
Correlation analyses
For each of the spatially explicit up-scaling approaches MTE1, MTE2, ANN, LUE, and KGB,
and for the median GPP of these approaches, we performed a partial correlation analysis be-
tween GPP and precipitation, air temperature and short-wave radiation. This analysis has been
done for 4.5◦ by 4.5◦ moving windows. The resolution of the data is 0.5◦ by 0.5◦ , i.e. for each
0.5◦ pixel, surrounding 81 pixels have been used. Additionally, three sets of climate variables
were applied: a) CRU air temperature, CRU precipitation and ECMWF ERA-Interim short-
wave radiation, b) ECMWF ERA-Interim air temperature, precipitation and short-wave radia-
tion, and c) CRU air temperature, GPCP precipitation and ECMWF ERA-Interim short-wave
radiation. Type b is the most consistent dataset, type c is most strongly based on observations,
and type a is in between these extremes: air temperature and precipitation are consistent and
based on observations.
In Tab. 2 and Fig. 3 of the main paper and in Tab. 6, Fig. 28 and Fig. 29 resulting significant
(p<0.01) correlations are shown. Fig. 2 of the main paper shows example maps for the case of
using the median GPP and climate set type a.
GPP-Climate correlations
50
(a) (b) (c)
(d) (e) (f)
Figure 28: Same as Fig. 3 of the main paper but complete for all climate variables.
(a) (b) (c)
(d) (e) (f)
Figure 29: Same as Fig. 28 but showing all model results individually.
51
Partial correlation LPJ GPP and precipitation
−1
−0.5
0
0.5
1
Partial correlation LPJ GPP and temperature
−1
−0.5
0
0.5
1
Partial correlation LPJ GPP and radiation
−1
−0.5
0
0.5
1
Figure 30: Partial correlation in the spatial domain between GPP from the LPJ-DGVM andeither CRU precipitation (above), CRU air temperature (middle), or ECMWF ERA-Interimshort-wave radiation (bottom) after applying a moving 4.5◦ by 4.5◦ spatial window and sub-sequent median filtering. Shown are significant correlations (p<0.01) of which the correlationcoefficient is higher/lower than ± 0.2.
52
Partial correlation LPJmL GPP and precipitation
−1
−0.5
0
0.5
1
Partial correlation LPJmL GPP and temperature
−1
−0.5
0
0.5
1
Partial correlation LPJmL GPP and radiation
−1
−0.5
0
0.5
1
Figure 31: Partial correlation in the spatial domain between GPP from LPJmL and either CRUprecipitation (above), CRU air temperature (middle), or ECMWF ERA-Interim short-wave ra-diation (bottom) after applying a moving 4.5◦ by 4.5◦ spatial window and subsequent medianfiltering. Shown are significant correlations (p<0.01) of which the correlation coefficient ishigher/lower than ± 0.2.
53
Partial correlation SDGVM GPP and precipitation
−1
−0.5
0
0.5
1
Partial correlation SDGVM GPP and temperature
−1
−0.5
0
0.5
1
Partial correlation SDGVM GPP and radiation
−1
−0.5
0
0.5
1
Figure 32: Partial correlation in the spatial domain between GPP from the SDGVM and eitherCRU precipitation (above), CRU air temperature (middle), or ECMWF ERA-Interim short-wave radiation (bottom) after applying a moving 4.5◦ by 4.5◦ spatial window and subsequentmedian filtering. Shown are significant correlations (p<0.01) of which the correlation coeffi-cient is higher/lower than ± 0.2.
54
Partial correlation ORC GPP and precipitation
−1
−0.5
0
0.5
1
Partial correlation ORC GPP and temperature
−1
−0.5
0
0.5
1
Partial correlation ORC GPP and radiation
−1
−0.5
0
0.5
1
Figure 33: Partial correlation in the spatial domain between GPP from ORCHIDEE and eitherCRU precipitation (above), CRU air temperature (middle), or ECMWF ERA-Interim short-wave radiation (bottom) after applying a moving 4.5◦ by 4.5◦ spatial window and subsequentmedian filtering. Shown are significant correlations (p<0.01) of which the correlation coeffi-cient is higher/lower than ± 0.2.
55
Partial correlation CLM GPP and precipitation
−1
−0.5
0
0.5
1
Partial correlation CLM GPP and temperature
−1
−0.5
0
0.5
1
Partial correlation CLM GPP and radiation
−1
−0.5
0
0.5
1
Figure 34: Partial correlation in the spatial domain between GPP from CLM-CN and either CRUprecipitation (above), CRU air temperature (middle), or ECMWF ERA-Interim short-wave ra-diation (bottom) after applying a moving 4.5◦ by 4.5◦ spatial window and subsequent medianfiltering. Shown are significant correlations (p<0.01) of which the correlation coefficient ishigher/lower than ± 0.2.
56
Table 6: Percentage of biome area that is climatically controlled, indicated by a partial cor-relation coefficient higher than 0.2 (or 0.5 in brackets). Columns 5 to 7 show the percentageof biome area with a negative partial correlation coefficient to the climate variables lower than-0.2 (or -0.5 in brackets). Here, CRU precipitation and temperature, and ECMWF ERA-Interim radiation was used for the correlation analysis.
Biome pos corr Pa pos corr Tb pos corr Rc neg corr P neg corr T neg corr R
Tropical forests 47 (26) 39 (26) 4 (1) 4 (1) 12 (3) 42 (21)
Temperate forests 66 (46) 43 (25) 6 (1) 3 (1) 5 (1) 38 (20)
Boreal forests 36 (19) 53 (30) 24 (9) 14 (5) 5 (1) 19 (7)
Tropical savannahs &grasslands
63 (43) 20 (7) 5 (1) 4 (1) 17 (3) 49 (25)
Temperate grasslands& shrublands
75 (53) 41 (21) 9 (3) 2 (1) 11 (3) 40 (19)
Deserts 70 (51) 26 (11) 7 (2) 2 (0) 13 (4) 34 (15)
Tundra 39 (26) 42 (30) 28 (12) 18 (9) 12 (6) 15 (7)
Croplands 66 (42) 29 (13) 7 (1) 2 (0) 12 (3) 39 (17)
aprecipitationbair temperaturecshort-wave radiation
57
Table 7: Percentage of biome area that is climatically controlled, indicated by a partial cor-relation coefficient higher than 0.2 (or 0.5 in brackets). Columns 5 to 7 show the percentageof biome area with a negative partial correlation coefficient to the climate variables lower than-0.2 (or -0.5 in brackets). Here, ECMWF ERA-Interim climate was used for the correlationanalysis.
Biome pos corr Pa pos corr Tb pos corr Rc neg corr P neg corr T neg corr R
Biome pos corr P pos corr T pos corr R neg corr P neg corr T neg corr R
Tropical forests 26 (12) 18 (10) 6 (1) 8 (2) 29 (12) 32 (14)
Temperate forests 53 (29) 37 (19) 10 (3) 1 (0) 9 (3) 25 (8)
Boreal forests 24 (7) 56 (31) 20 (6) 13 (4) 1 (0) 19 (6)
Tropical savannahs &grasslands
46 (24) 15 (6) 6 (2) 7 (1) 29 (10) 48 (25)
Temperate grasslands& shrublands
66 (41) 38 (20) 9 (3) 2 (0) 9 (2) 35 (14)
Deserts 57 (36) 19 (6) 12 (3) 3 (0) 19 (10) 24 (9)
Tundra 20 (10) 39 (25) 32 (14) 19 (8) 10 (4) 10 (4)
Croplands 48 (22) 24 (10) 7 (1) 3 (0) 14 (4) 30 (12)
aprecipitationbair temperaturecshort-wave radiation
58
Table 8: Percentage of biome area that is climatically controlled, indicated by a partial cor-relation coefficient higher than 0.2 (or 0.5 in brackets). Columns 5 to 7 show the percentageof biome area with a negative partial correlation coefficient to the climate variables lower than-0.2 (or -0.5 in brackets). Here, GPCP precipitation, CRU temperature, and ECMW ERA-Interim radiation was used for the correlation analysis, and the median reported.
Biome pos corr Pa pos corr Tb pos corr Rc neg corr P neg corr T neg corr R
Biome pos corr P pos corr T pos corr R neg corr P neg corr T neg corr R
Tropical forests 24 (10) 46 (35) 5 (1) 7 (2) 15 (4) 43 (24)
Temperate forests 34 (16) 44 (30) 10 (3) 10 (4) 12 (5) 35 (18)
Boreal forests 15 (4) 55 (34) 25 (9) 23 (10) 5 (1) 16 (5)
Tropical savannahs &grasslands
51 (29) 18 (8) 3 (0) 5 (1) 29 (11) 47 (22)
Temperate grasslands& shrublands
54 (33) 32 (18) 9 (2) 6 (2) 22 (9) 37 (16)
Deserts 51 (29) 15 (6) 14 (5) 3 (1) 30 (15) 26 (12)
Tundra 23 (12) 36 (28) 40 (21) 20 (10) 27 (18) 10 (4)
Croplands 40 (20) 34 (22) 8 (2) 8 (3) 20 (7) 40 (19)
aprecipitationbair temperaturecshort-wave radiation
59
Table 9: List of FLUXNET sites used
Site Vegetation type ReferenceAT-Neu GRA (72)AU-Fog WET -AU-Tum EBF (73)AU-Wac EBF (74)BE-Bra MF (75)BE-Lon CRO (76)BE-Vie MF (77)BR-Ban EBF -BR-Ji2 GRA (78)BR-Ma2 EBF (79)BR-Sa1 EBF (80)BR-Sa2 CRO (81)BR-Sa3 EBF (82)BR-Sp1 WSA (83)BW-Ma1 WSA (84)CA-Ca1 ENF (85)CA-Ca2 ENF (85)CA-Ca3 ENF (85)CA-Let GRA (86)CA-Man ENF (87)CA-Mer OSH (88)CA-NS1 ENF (89)CA-NS3 ENF (89)CA-NS6 OSH (89)CA-NS7 OSH (89)CA-Oas DBF (90)CA-Obs ENF (91)CA-Ojp ENF (92)CA-Qcu ENF (93)CA-Qfo ENF (91)CA-SJ1 ENF (94)CA-SJ2 ENF (94)CA-SJ3 ENF (94)CA-TP4 ENF (95)CA-WP1 MF (96)CH-Oe1 GRA (97)CH-Oe2 CRO (98)CN-Cha MF (99)
60
CN-Do1 WET (100)CN-Do2 WET (100)CN-Do3 WET (100)CN-HaM GRA (101)CN-Xfs GRA -DE-Bay ENF (102)DE-Geb CRO (103)DE-Gri GRA (104)DE-Hai DBF (105)DE-Har ENF (106)DE-Kli CRO -DE-Meh MF (107)DE-Tha ENF (108)DE-Wet ENF (109)DK-Lva GRA (104)DK-Ris CRO (110)DK-Sor DBF (111)ES-ES1 ENF (112)ES-ES2 CRO -ES-Lma SAV -ES-VDA GRA (104)FI-Hyy ENF (113)FI-Sii GRA (114)FI-Sod ENF (115)FR-Fon DBF -FR-Gri CRO (116)FR-Hes DBF (117)FR-LBr ENF (118)FR-Lq1 GRA (104)FR-Lq2 GRA (104)FR-Pue EBF (119)GF-Guy EBF (120)HU-Bug GRA (121)HU-Mat GRA (122)ID-Pag EBF (123)IE-Dri GRA -IL-Yat ENF (124)IT-Amp GRA (104)IT-Bci CRO (125)IT-Cpz EBF (126)IT-Lav ENF (127)
61
IT-Lec EBF -IT-Mbo GRA (128)IT-PT1 EBF (129)IT-Ren ENF (130)IT-Ro1 DBF (131)IT-Ro2 DBF (132)IT-SRo ENF (133)JP-Mas CRO (134)JP-Tak DBF (135)JP-Tef MF (136)JP-Tom MF (137)NL-Hor GRA (138)NL-Loo ENF (139)PL-Wet WET (140)PT-Mi1 EBF (141)PT-Mi2 GRA (141)RU-Fyo ENF (142)SE-Deg WET (143)SE-Fla ENF (144)SE-Nor ENF (145)UK-Gri ENF (146)UK-Ham DBF -UK-PL3 DBF -US-ARM CRO (147)US-Aud GRA -US-Bar DBF (148)US-Bkg GRA (149)US-Blo ENF (150)US-Bn2 DBF (151)US-Bo1 CRO (152)US-Bo2 CRO (152)US-Dk3 MF (153)US-Fpe GRA -Site Vegetation type ReferenceUS-FR2 WSA (154)US-Goo GRA -US-Ha1 DBF (155)US-Ho1 ENF (156)US-Ho2 MF (156)US-IB1 CRO (157)US-IB2 GRA (157)
62
US-KS2 CSH (158)US-LPH DBF (159)US-MMS DBF (160)US-Moz DBF (161)US-Me4 ENF (162)US-NC1 OSH (163)US-NC2 ENF (164)US-NR1 ENF (165)US-Ne1 CRO (166)US-Ne2 CRO (166)US-Ne3 CRO (166)US-Pfa MF (167)US-SO2 WSA (168)US-SO3 WSA (168)US-SO4 CSH -US-SP1 ENF (169)US-SP2 ENF (170)US-SP3 ENF (170)US-SRM WSA (171)US-Ton WSA (172)US-UMB DBF (173)US-Var GRA (174)US-WBW DBF (175)US-WCr DBF (176)US-Wrc ENF (177)VU-Coc EBF (178)
63
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