12 | | Instantaneous fields and the LongWave Radiation are then linearly interpolated for each t:t+1 time period in order to calculate half-hourly value. |
13 | | The Precipitation field is downscaled to half-hourly resolution using a step distribution function with one parameter (spread_prec). |
| 13 | * Interpolation |
| 14 | * Instantaneous fields and the Long-Wave Radiation are then linearly interpolated for each t:t+1 time period in order to calculate half-hourly value. |
| 15 | * The Precipitation field is downscaled to half-hourly resolution using a step distribution function with one parameter (nb_spread, that is the number of half-hourly time steps over which we spread the precipitation). nb_spread can vary from 1 (all precipitations over a forcing time period (3 ou 6 hours) are put on the first time step) to SPLIT_DT (number of integration time steps with a forcing time period, in that case, the precipitation are distributed uniformely). By default, nb_spread is set to 1. |
| 16 | * The Short-Wave radiation is interpolated using a function distribution that corresponds to the solar angle distribution over a forcing time period. |
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| 19 | == Add an explicit time information within the forcing files == |
| 20 | As described above, the driver of ORCHIDEE is relatively rigid because it only assumes one temporal specification for the forcing files. At first, we do not expect to develop a more flexible driver but we would like to add explicit time information in the driver in order to avoid misuse. |
| 21 | We suggest to add time_bounds attributes to the variables stored in the NetCdf forcing files. |
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