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Note that in the tables below, "an" and "fc" is just a label used for convention to archive the data in MARS.
Table 1: stream=oper/mnth/moda, levtype=sfc: surface parameters: instantaneous
name | units | Variable name in CDS | shortName | paramId | an | fc | GRIB1 | GRIB2 | Used as forcing field | |
---|---|---|---|---|---|---|---|---|---|---|
1 | K | lake_mix_layer_temperature | lmlt | 228008 | x | x | ||||
2 | m | lake_mix_layer_depth | lmld | 228009 | x | x | ||||
3 | K | lake_bottom_temperature | lblt | 228010 | x | x | ||||
4 | K | lake_total_layer_temperature | ltlt | 228011 | x | x | ||||
5 | dimensionless | lake_shape_factor | lshf | 228012 | x | x | ||||
6 | K | lake_ice_temperature | lict | 228013 | x | x | ||||
7 | m | lake_ice_depth | licd | 228014 | x | x | ||||
8 | Snow cover | % | snow_cover | snowc | 260038 | x | x | |||
9 | Snow depth | m | snow_depth | sde | 3066 | x | x | |||
10 | (0 - 1) | snow_albedo | asn | 32 | x | x | ||||
11 | kg m**-3 | snow_density | rsn | 33 | x | x | ||||
12 | m**3 m**-3 | volumetric_soil_water_layer_1 | swvl1 | 39 | x | x | ||||
13 | m**3 m**-3 | volumetric_soil_water_layer_2 | swvl2 | 40 | x | x | ||||
14 | m**3 m**-3 | volumetric_soil_water_layer_3 | swvl3 | 41 | x | x | ||||
15 | m**3 m**-3 | volumetric_soil_water_layer_4 | swvl4 | 42 | x | x | ||||
16 | m**2 m**-2 | leaf_area_index_low_vegetation | lai_lv | 66 | x | x | ||||
17 | m**2 m**-2 | leaf_area_index_high_vegetation | lai_hv | 67 | x | x | ||||
18 | Pa | surface_pressure | sp | 134 | x | x | x | |||
19 | K | soil_temperature_level_1 | stl1 | 139 | x | x | ||||
20 | m of water equivalent | snow_depth_water_equivalent | sd | 141 | x | x | ||||
21 | m s**-1 | 10m_u_component_of_wind | u10 | 165 | x | x | x | |||
22 | m s**-1 | 10m_v_component_of_wind | v10 | 166 | x | x | x | |||
23 | K | 2m_temperature | 2t | 167 | x | x | ||||
24 | K | 2m_dewpoint_temperature | 2d | 168 | x | x | ||||
25 | K | soil_temperature_level_2 | stl2 | 170 | x | x | ||||
26 | K | soil_temperature_level_3 | stl3 | 183 | x | x | ||||
27 | m of water equivalent | skin_reservoir_content | src | 198 | x | |||||
28 | K | skin_temperature | skt | 235 | x | x | ||||
29 | K | soil_temperature_level_4 | stl4 | 236 | x | x | ||||
30 | K | temperature_of_snow_layer | tsn | 238 | x | x | ||||
31 | (0 - 1) | forecast_albedo | fal | 243 | x | x |
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2 Leaf Area Index (LAI) parameters are based on a monthly climatology as explained IFS model documentation CY45R1. So the user will only see monthly variability, but not inter-annual variability.
Table 2: stream=oper/mnth/moda, levtype=sfc: surface parameters: accumulations
name | units | Variable name in CDS | shortName | paramId | an | fc | GRIB1 | GRIB2 | Used as forcing field | |
---|---|---|---|---|---|---|---|---|---|---|
1 | m | surface_runoff | sro | 8 | x | x | ||||
2 | m | sub_surface_runoff | ssro | 9 | x | x | ||||
3 | m of water equivalent | snowmelt | smlt | 45 | x | x | ||||
4 | m of water equivalent | snowfall | sf | 144 | x | x | x | |||
5 | Surface sensible heat flux | J m**-2 | surface_sensible_heat_flux | sshf | 146 | x | x | |||
6 | Surface latent heat flux | J m**-2 | surface_latent_heat_flux | slhf | 147 | x | x | |||
7 | Surface solar radiation downwards | J m**-2 | surface_solar_radiation_downwards | ssrd | 169 | x | x | x | ||
8 | Surface thermal radiation downwards | J m**-2 | surface_thermal_radiation_downwards | strd | 175 | x | x | x | ||
9 | Surface net solar radiation | J m**-2 | surface_net_solar_radiation | ssr | 176 | x | x | x | ||
10 | Surface net thermal radiation | J m**-2 | surface_net_thermal_radiation | str | 177 | x | x | x | ||
11 | m of water equivalent | total_evaporation | e | 182 | x | x | ||||
12 | m | runoff | ro | 205 | x | x | ||||
13 | m | total_precipitation | tp | 228 | x | x | x | |||
14 | Evaporation from the top of canopy | m of water equivalent | evaporation_from_the_top_of_canopy | evatc | 228100 | x | x | |||
15 | Evaporation from bare soil | m of water equivalent | evaporation_from_bare_soil | evabs | 228101 | x | x | |||
16 | Evaporation from open water surfaces excluding oceans | m of water equivalent | evaporation_from_open_water_surfaces_excluding_oceans | evaow | 228102 | x | x | |||
17 | Evaporation from vegetation transpiration | m of water equivalent | evaporation_from_vegetation_transpiration | evavt | 228103 | x | x | |||
18 | m | potential_evaporation | pev | 228251 | x | x |
Accumulations are described in section 140385203 ERA5-Land: data documentation#accumulations. The accumulations in monthly means (stream=moda/mnth) are described in section monthly means
How to use lake-related fields
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The ECMWF model also contains an ice module, a snow module and a bottom sediments module. The present setup of the IFS is running with no bottom sediment and snow modules (snow accumulation over ice is not allowed and snow parameters are used only for albedo purposes). In the implementation in the IFS lake ice can be fractional within a grid-box with inland water (10 cm of ice means 100 % of a grid-box or tile is covered with ice; 0 cm of ice means 100 % of the grid-box is covered by water; in between a linear interpolation is applied) (Manrique-Sunen et al., 2013). At present, the water balance equation is not included for lakes and the lake depth and surface area are kept constant in time (IFS Documentation, 2017, chapter 8 and 11 ). Lake parametrization also requires the lake fraction CL, lake depth DL (preferably bathymetry), and lake initial conditions. DL is the most important external parameter that uses the lake parametrization.
Known issues
Expand title Uncertainty fields As it was done for ERA5, the original plan for ERA5-Land was to provide an estimate of the uncertainty fields based on a dedicated 10-member ensemble run. The latter generated an ensemble of forcing fields that should, in principle, reproduce the space of uncertainty for the land surface fields. The first experiments demonstrated that the spread of the ensemble was clearly under dispersive, i.e. the uncertainty was unrealistically low. A reason for this is the low spread shown by the ensemble of ERA5 forcing fields.
As a result of these experiments we took the decision of not providing the uncertainty fields of ERA5-Land. The opposite would have assigned, for instance, unrealistically high confidence to ERA5-land fields in a data assimilation experiment.
Our recommendation is, for the time being, to use the uncertainty estimate of the corresponding ERA5 field, which should provide a second order approximation to the estimate of the real uncertainty. Future experiments will also perturbe, among other, key land surface model parameters, therefore providing a more realistic spread of the ERA5-Land ensemble surface fields.
Three components of the total evapotranspiration have values swapped as follows:
- variable "Evaporation from bare soil" (mars parameter code 228101 (evabs)) has the values corresponding to the "Evaporation from vegetation transpiration" (mars parameter 228103 (evavt)),
- variable "Evaporation from open water surfaces excluding oceans (mars parameter code 228102 (evaow)) has the values corresponding to the "Evaporation from bare soil" (mars parameter code 228101 (evabs)),
- variable "Evaporation from vegetation transpiration" (mars parameter code 228103 (evavt)) has the values corresponding to the "Evaporation from open water surfaces excluding oceans" (mars parameter code 228102 (evaow)).Expand title Low values of snow cover and snow depth on the eastern side of the Antarctic ice sheet Low values of snow cover and snow depth were found on the eastern side of the Antarctic ice sheet, as shown in Fig. 1. The issue is due to the application of an old glacier mask to the Antarctica, which excludes the patch shown in the figure as glacier. Inaccuracies in the glacier mask are due to errors in satellite measurements datasets. While, due to the lower horizontal resolution, in ERA5 this ice sheet part is a sea point, in ERA5-Land the area is categorised as land without an initial ice mass. Since the initialization doesn't consider a glacier there (estimated at a constant 10 m of snow water equivalent), the low amount of precipitation along with potential excess of sublimation makes them to obtain unrealistic low numbers there.
Fig 1: ERA-Land Snow depth (m of water equivalent) on 01-01-2015 eastern side of the Antarctic ice sheet.
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