Agricultural and Forest Meteorology 98±99 (1999) 257±277 Validation of a distributed hydrological model against spatial observations Yuri G. Motovilova,*,1, Lars Gottschalka, Kolbjùrn Engelanda, Allan Rodheb a Department of Geophysics, University of Oslo, PO Box 1022, Blindern, 0315 Oslo, Norway b Department Hydrology, Institute of Earth Sciences, Uppsala, Sweden Abstract In connection with climate change studies a new hydrologic ®eld has evolved Ð regional hydrological modelling or hydrologic macro modelling, which implies repeated application of a model everywhere within a region using a global set of parameters. The application of a physically based distributed hydrological model ECOMAG to river basins within the NOPEX southern region with this purpose in mind is presented. The model considers the main processes of the land surface hydrological cycle: in®ltration, evapotranspiration, heat and water regime of the soil, snowmelt, formation of surface, subsurface and river runoff and groundwater. The spatial integration of small and meso-scale non-homogeneity of the land surface is a central issue both for the de®nition of fundamental units of the model structure and for determination of representative values for model validation. ECOMAG is based on a uniform hydrological (or landscape) unit representation of the river basin, which re¯ects topography, soil, vegetation and land use. As a ®rst step the model was calibrated using standard meteorological and hydrological data for 7 years from regular observation networks for three basins. An additional adjustment of the soil parameters was performed using soil moisture and groundwater level data from ®ve small experimental basins. This step was followed by validation of the model against runoff for 14 years from six other drainage basins, and synoptic runoff and evapotranspiration measurements performed during two concentrated ®eld efforts (CFEs) of the NOPEX project in 1994 and 1995. The results are promising and indicate directions for further research. # 1999 Elsevier Science B.V. All rights reserved. Keywords: Hydrological model; Evapotranspiration; NOPEX 1. Introduction Hydrological models account for the storage and ¯ow of water on the continents, including exchanges of water and energy with the atmosphere and oceans. During the past three decades, hydrologists have developed a large number of models ranging in sophis* 1 Corresponding author. On leave from Institute for Applied Ecology, Moscow, Russia. tication and complexity. Most of these models apply to geographical areas smaller than the area represented by a typical GCM grid square, although some basinscale hydrological models have been applied to areas as large as 104 km2. `Macro-scale' hydrological models are hydrological models that are compatible with the scale of a GCM grid square (e.g. 105 km2) and can accept atmospheric model data as input. Preparing macro-scale hydrological models is a major undertaking that will require the co-operative 0168-1923/99/$ ± see front matter # 1999 Elsevier Science B.V. All rights reserved. PII: S 0 1 6 8 - 1 9 2 3 ( 9 9 ) 0 0 1 0 2 - 1 258 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 effort of hydrologists and other geo-scientists all over the world. The challenge is to extend existing knowledge of hydrological processes, as they occur at a point location and on the scale of small basins, to the macro-scale. Macro-scale hydrological models must be able to exchange information with atmospheric models. Processes that occur at a sub-grid scale must be accounted for internally in these hydrological models. Ultimately, it must be possible to apply the model globally. There are no data to calibrate macroscale hydrological models in the same way that hydrologists usually calibrate catchment models. Therefore, the required macro-scale models must account for the water balance of `ungauged areas', and model parameters must be estimated a priori using limited climate, soil and vegetation data. Among the general requirements of hydrological models designed to assess the sensitivity of water resources to climate processes (Klemes, 1985) are the following: 1. They must be geographically transferable and this has to be validated in the real world; 2. Their structure must have a sound physical foundation and each of the structural components must permit its separate validation. Klemes (1986) presents a hierarchical scheme for systematic testing of the grounds for credibility of a given hydrological model and this is the scheme followed here. Most models applied by hydrologists in climate change studies at present are poorly adapted to the problem they are aimed to solve. The critical problem is that they are often lumped (semi-distributed) with calibrated `effective' parameters. This fact seriously hinders approaching the issue of scale (aggregation/ disaggregation) that is the focal scienti®c problem. Thus, a new hydrologic research ®eld has evolved Ð regional hydrological modelling or hydrologic macromodelling. This new concept implies an application of a hydrological model over a large spatial domain (at least 105 km2) or, more precisely, the repeated application of a model everywhere within this domain. There are two approaches to the development of a macro-model (Arnell, 1993): 1. `Top-down' which treats each of the fundamental units as a single drainage basin, and applies to each of them a lumped catchment model (the classical example is the Budyko bucket model and its modi®cations, Korzun, 1978, more recent ones are provided by VoÈroÈsmarty et al., 1989; VoÈroÈsmarty and Moore, 1991; DuÈmenil and Todini, 1992, Sausen et al., 1994). 2. `Bottom-up' which identi®es representative hydrological areas and aggregates upwards to the fundamental unit size (see `scale issues' below) For the latter approach, data for validation of the process description are essential. Of great importance in this context is a series of recent and ongoing land surface experiments, where hydrologists together with meteorologists, climatologists, plant physiologists, ecologists, soil scientists, geohydrologists etc. study exchange processes between the land surface and the atmosphere at a range of scales, from an individual soil column with vegetation to the globe as a whole. The design and execution of these coordinated experiments constitute a landmark in hydrology realising that the essence of physical science is experimentation (National Research Council, 1991). Historically most hydrologic data have been collected to answer water resources questions rather than scienti®c ones. The most critical barrier to future development of theoretical hydrology is the availability of data for identifying and verifying theories (Gottschalk and Askew, 1987). The recent and ongoing land surface experiments provide us with such data. Here data from the northern hemisphere climate processes land-surface experiment (NOPEX) (Halldin et al., 1995, 1999) are utilised for calibration and validation of a physically based distributed hydrological model ECOMAG (Motovilov et al., 1999). The NOPEX study region is chosen to represent northern landscapes such as the boreal forests, which play an important role in global hydrological and biogeochemical cycles (Thomas and Rowntree, 1992). The NOPEX area is situated in southern Sweden, in the densest part of the northern European boreal forest zone. The NOPEX region is also centrally situated in the Baltic Sea drainage basin, which is the study region for the BALTEX project. The validation of the ECOMAG model performed here is a test of its ability to live up to the demands for a macro hydrological model. The following steps have been de®ned: Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 Calibration of the model against runoff for three basins with one global set of parameters. Adjustment of the soil parameters of the model against soil moisture and groundwater level data from five small experimental sub-basins. Validation against synoptic measurements of runoff. Validation against runoff in six other basins that are not used for calibration. Validation against regional flux estimates (evapotranspiration) for the whole NOPEX region. The task put forward is demanding and it can hardly be expected that a model will perform well in relation to all tests undertaken. The results of the validation will however point to critical issues indicating how the model process formulation and parameterisation can be improved. An introductory part of the paper presents in brief the main features of the ECOMAG model and the basic datasets used for model calibration and validation. The scale issue is of importance for de®nition of the spatial grid resolution of the model and for comparing data measured at `points' with modelled data representing grid cells. These aspects are discussed ®rst to give a background to the model formulation and also to the description of the validation procedure. Finally, some conclusions based on the gained experience are drawn. 2. NOPEX The model development is centred on data from the NOPEX experiment, performed north of the city of Uppsala in southern Sweden. The southern NOPEX region is an area of low relief with heterogeneous surface cover, represented by coniferous and mixed forest (57%), open land (mainly agricultural) (35.8%), mires (2.6%), lakes (2.6%) and urbanised areas (2.0%) (evaluated from digital maps of the National Land Survey of Sweden). The area is therefore very suitable for studying the inter- and intra-patch variability of energy and mass exchange processes. An extensive amount of meteorological and hydrological data collected during the NOPEX concentrated ®eld efforts (CFE) CFE1 (27 May±23 June 1994) and CFE2 (18 April±14 July 1995) has been utilised in the 259 process of setting up the model, its calibration and validation: Geographical data including a digital terrain model with a resolution of 50 m and land use data with 25 m resolution (both datasets from the National Land Survey of Sweden) and a comprehensive digitised soil map with a resolution of 2 km (from Seibert, 1994). The regular hydrological discharge observation network run by the Swedish Meteorological and Hydrological Institute (SMHI). The NOPEX area contains 11 standard gauging stations in drainage basins covering the main part of the area (Fig. 1) which provided 24 h average values for the period 1981±95. Data (daily values) from 25 precipitation stations, 7 temperature stations and 5 stations for vapour pressure deficit for the period 1981±95 from the regular climatic observation network run by SMHI were used. The temperature and vapour pressure deficit were interpolated to a regular 2 km grid by inverse distance weighting and the precipitation was interpolated by kriging. Detailed hydrological studies concentrated in five experimental basins (see Fig. 1 for location) during the NOPEX CFE1 and CFE2. These included measurements of discharge, groundwater levels and soil moisture as well as standard climatological variables. The sites for groundwater levels and soil moisture measurements were chosen to represent different geomorphologic units (hollow, slope, and nose) within the experimental basins. This dataset comprises about 2000 individual measurements of groundwater levels and about 16 000 measurements of soil moisture content (the measurements were also performed outside CFE periods) (Tallaksen et al., 1999). Synoptic discharge measurements at 38 sites in the FyrisaÊn river basin on four occasions during recession. The procedure for these measurements followed that reported by Krasovskaia (1988) and Rodhe et al. (1999). 3. Scale issues An ambition within the NOPEX project is to bring insight into the scale of variation. For this purpose 260 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 Fig. 1. The NOPEX area showing the nine gauged drainage basins and five experimental basins. spatial data for the NOPEX area (digital terrain data: topography, land use, soil types and remotely sensed data) have been analysed with respect to homogeneity, uniformity, correlation lengths and the effect of spatial aggregation (scaling) on these properties (Sulebakk, 1997). Soil moisture, groundwater and synoptic runoff measurements were analysed with the aim of identifying spatial scales (patches, representative areas) of relevanceforaggregationapproaches(Beldringetal.,1999). In meteorology and also in subsurface hydrology there is a tradition of distinguishing between spatial variability at different scales. In surface hydrology it is quite a recent way of thinking. The concept of representative elementary volume (REV) on which scale basic theoretical equations are founded is focal in this respect. Wood et al. (1988, 1990) have introduced the complementary concept of representative elementary area (REA). At a certain scale a landscape element (a drainage basin or a grid cell) might contain a suf®cient sample of the geomorphologic, soil and other relevant characteristics of the region. It is then no longer necessary to take account of the pattern of those characteristics but only of their distribution. The underlying variability may still be important in controlling both discharges and evaporation ¯uxes, but the patterns are less important. The scale at which this happens de®nes the REA. The REA concept is not a direct analogy with the REV in subsurface hydrology as the REV denotes a scale at which average quantities of potential and moisture content can be used in a continuum description of the ¯uxes. In the REA the distribution of characteristics may still be important in determining the ¯uxes. Fig. 2 shows examples of plots used to identify the REA for terrain with till soils. The soil moisture and groundwater level data were obtained by the measurements in the NOPEX area during CFEs periods. A preliminary conclusion is that for this type of terrain the main part of the spatial variability in soil moisture and groundwater ¯uctuations is contained in the 2 km Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 261 Fig. 2. Spatial variation of soil moisture and groundwater levels as a function of scale of aggregation (from Beldring et al., 1999). grid size used for modelling (Beldring et al., 1999). Theoretical distribution functions have been developed that can take into account this variability. The possibility of identifying a REA is of vital importance for the process formulation in the ECOMAG model as it indicates that within a grid cell of 2 km runoff is delivered to the river network and that rivers provide the only exchange between grid cells in this type of landscape. The exchange through groundwater ¯ow is of negligible order, as there are no runoff formation factors acting at a between grid cell scale (no signi®cant gradients in soil moisture content and groundwater levels between grid cells at this scale). From the scale analysis it is obvious that measured soil moisture and groundwater level values cannot be compared directly with the corresponding modelled ones. The latter values do not re¯ect the full small scale variability as illustrated by the left-hand side of the diagrams in Fig. 2. Measured data must be averaged to the REA scale to be able to match model output. 4. Hydrological model formulation Distributed hydrological models allow the determination of the water balance and its variation across river basins. Several such models are in common use (i.e. SHE-model, Abbott et al., 1986; TOPMODEL, Beven and Kirkby, 1979; WATBAL Knudsen et al., 1986) but none of them explicitly contains components re¯ecting important characteristics of the boreal landscape like mires, lakes and the close relationship between soil moisture and groundwater in the till soil. Preliminary analyses of surveys of runoff data indicate that the main factors, which explain the spatial variation in runoff, are the frequency of lakes and mires in upstream areas (Erichsen et al., 1995). Consequently, a distributed hydrological model ECOMAG (Motovilov and Belokurov, 1997; Motovilov et al., 1999) developed for application to boreal conditions was used. The model describes the processes of soil in®ltration, evapotranspiration, thermal and water regimes of the soil, surface and subsurface ¯ow, groundwater 262 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 and river ¯ow, snow accumulation and snowmelt. In its original form a drainage basin is approximated by irregular triangular or trapezoidal elements, taking into consideration peculiarities of topography (size, form and slope), soil types (peat, clay, sand, till, bedrock), vegetation and land use (open area, forest, lake, mire, urban area) in a GIS framework. This version of the model has already been applied and tested in Russia. It is based on 15-year's experience of the development and application of distributed physically based hydrological models (Kuchment et al., 1983, 1986, 1989; Motovilov, 1986, 1987, 1993). A second version of the model is now under development (Gottschalk et al., 1998) and the present paper is a step in this new direction. The main change is the use of a regular grid network (2 km 2 km) in order to, with further development, allow direct coupling with a meso-scale meteorological model and the use of radar-evaluated precipitation data (Crochet, 1999). The basic assumption of the model is that a river basin can be sub-divided into a mosaic of irregular or regular elements, each to be viewed as a landscape hydrological unit. The REA concept referred to above is of vital importance here as it constitutes a minimum size for such an element. The speci®c characteristics of topography, structure of river network, soil types, land use etc. for each element are determined in a GIS framework. The hydrological model for a landscape unit was constructed in conformity with the following scheme taking into account the processes of hydrological cycle (Fig. 3). During a summer period the rain partially in®ltrates into the soil and penetrates into Fig. 3. Block-scheme of the ECOMAG model structure for a fundamental landscape unit. Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 deeper soil layers. The soil is divided into a top layer (horizon A), an intermediate layer (horizon B) and a bottom layer (groundwater storage). The total porosity of the soil is divided into two parts: a capillary zone (the upper limit of which is the ®eld capacity) and a noncapillary zone (the difference between total porosity and ®eld capacity). After the ®lling of depressions on the surface, the excess of water, not absorbed by the soil, runs off on the sloping land surface to the river network (surface ¯ow). A part of the water, which was in®ltrated into the soil, follows a temporary, relatively impermeable, boundary along the slopes as shallow groundwater (subsurface) ¯ow. Another part is transported in the groundwater zone and forms base ¯ow. The subsurface and groundwater ¯ow is modelled as a Darcy ¯ow, while the surface and river runoff is described by a simpli®ed version of the kinematic wave equation (Rose et al., 1983). Under the condition of high soil moisture content, the actual evaporation equals the potential, and then linearly decreases with the decay of the soil moisture content to a certain lowest level, being zero at the soil moisture content equal to the wilting point (Feddes et al., 1974). Lake-element in the area is described as a storage with recession coef®cient de®ned on the basis of the kinematic wave equation. The actual evaporation is taken equal to the potential one. During cold periods of the year, the scheme is supplemented by hydrothermal processes Ð snow cover formation, snowmelt, freezing and thawing of the soil, and in®ltration of snowmelt water into the frozen soil. The phase composition of precipitation is determined by the daily average air temperature. The snowmelt rate is calculated using the degree-day method. Evaporation of solid and liquid phases of snow is estimated using data on vapour pressure de®cit. It is assumed that the vertical temperature pro®les in the snow as well as in the frozen and thawed soil differ only slightly from linear ones, and that the migration of moisture to the freezing front is negligible. Under these conditions the soil-frost and soil-thawing depth dynamics can be described by a system of ordinary differential equations (Motovilov and Nazarov, 1991). In®ltration of rain and meltwater into the frozen soil is calculated, taking into account the in¯uence of ice 263 content in the frozen soil on the hydraulic conductivity of the soil. The landscape information extracted from the GIS only grasps large scale features. Small scale ¯uctuations in landscape characteristics, however, are important for the runoff formation processes. A common approach in lumped hydrological models is to resolve this variability in terms of spatial distribution functions (Kuchment et al., 1986). A simpli®cation is to use the same distribution for all elements only allowing its mean value to vary between elements. In ECOMAG the within element variability is taken into consideration in this manner for three parameters Ð the vertical saturated hydraulic conductivity of soils, surface depression storage and soil ®eld capacity. For the ®rst two parameters an exponential function is applied (Popov, 1979; Vinogradov, 1988) and for the third Ð a parabolic function (BergstroÈm, 1976; DuÈmenil and Todini, 1992). 5. Model calibration procedure Many of the equations in a physically based model contain parameters and coef®cients that have a direct physical interpretation and, in principal, can be measured in the ®eld. Such parameters of the ECOMAG model are, in particular, the soil parameters with the exception of the horizontal hydraulic conductivity (Table 1). The initial values of these parameters for the different soil types were determined on the basis of regional information of agrohydrological properties of soils, supplemented by data from Nyberg (1995) and StaÈhli et al. (1996). For other parameters, experimental results have allowed the establishment of empirical relations (heat conductivity of soil and snow) or indicated reasonably well de®ned limits for parameter values (degree-day factor for snowmelt). In still other cases, the limits are not so well de®ned (for example, horizontal hydraulic conductivity for the calculation of shallow groundwater ¯ow) and these parameter values must be determined by calibration. The fact that not all parameters are well de®ned originates from scale issues and inadequacies in the model description. The various groups of parameters in the model may be calibrated in separate steps using only data about the dynamics of evapotranspiration, soil moisture, 264 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 Table 1 Model calibration parametersa Snow routine Degree-day factor Threshold temperature* Water holding capacity* Parameter of snow compaction* Soil routine Depth of horizon A Porosity Field capacity Wilting point Vertical hydraulic conductivity Horizontal hydraulic conductivity Factor for potential evaporation* Surface runoff routine Surface retention storage Surface roughness (Manning coefficient) River runoff routine River bed roughness (Manning coefficient)* a Parameters with asterisk (*) have one unique value for the whole NOPEX area, while the others have different values for different soil and land use types. groundwater, snow cover, frozen soil and river runoff, respectively. As a ®rst step in the calibration procedure the soil water parameters for different soil types were adjusted using soil moisture and groundwater level data on ®ve experimental river basins in the NOPEX area during 1994±95 including CFE periods. These basins were considered as the REA units representing different landscapes. The adjustment was carried out by manual inspection by means of a visual comparison of simulated and observed dynamics of soil moisture and groundwater levels. In a second step, the remaining model parameters were calibrated against runoff. This latter calibration and evaluation of the performance of ECOMAG were done using the Nash±Sutcliffe ef®ciency measure R2 (Nash and Sutcliffe, 1970). InP this the sum of squared residuals is de®ned q0 ÿq2 where F2 is the index of disagreeas: F 2 ment and q and q0 are the observed and computed discharges at corresponding times. F2 is analogous to the residual variance of a regression analysis. The sum is taken over a selected time period. The initial P qÿ q2 where q variance,F02 , is de®ned by F02 is the mean of the observed q and the sum is taken as before. It can be interpreted as the total variance of the data. This enables the ef®ciency of a model to be de®ned by R2 as the proportion of the initial variance accounted for by that model. R2 F02 ÿF 2 F02 (1) This R2 is analogous to the explained variance (the squared multiple correlation coefficient) in multiple regression. In regression analysis R2 can take values between zero and one only. Zero is the worst model fit when all the computed values are equal to the mean value q. The best value, one, is gained when the sum of squared residuals is zero. The calibration of a dynamic model is not directly analogous to a regression problem and the squared sum of residuals can, in principle, be higher than the variance of the data. The possible theoretical range for R2 is thus from minus infinity to one. A negative value would indicate a very bad model performance while values near to one indicate a good performance. The calibration of the model parameters against discharge data was done simultaneously for a number of river basins with different conditions of runoff formation to ®nd a global parameter set for the whole NOPEX area. The calibration was performed using a Rosenbrock optimisation procedure (Rosenbrock, 1960). The criterion of optimisation was calculated as a mean value of R2 for these river basins during the optimisation period. 6. Results of calibration and validation 6.1. Runoff at gauging stations Calibration of model parameters against runoff was carried out in three river basins, different in size and conditions of ¯ow formation: FyrisaÊn (at Ulva Kvarn) with an area of 950 km2; LillaÊn (at GraÈnvad) with an area of 168 km2and StabbybaÈcken (at Stabby) with an area of 6.2 km2. Seven years of observation were used in the calibration: 1986±93. These years were the most dif®cult for modelling with the presence a number of years with low annual ¯ow and unstable winters. The remaining 7 years of observations were used for the validation purposes. Table 2 contains an overview of the model ef®ciency R2 for all basins and all years, a total of 136 station years. Of these 21 have been used for calibration (marked with bold in the table) and the Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 265 Fig. 4. Calibration model runs for FyrisaÊn, LillaÊn and StabbybaÈcken. rest for validation. Fig. 4, showing observed and modelled hydrographs, illustrates the model performance for basins and years used for calibration. Satisfactory agreement between the observed and simulated runoff has been obtained. The model performance is better for 1986/87 than for 1988/89 in all three catchments. This re¯ects that when the simulations are wrong, often the same error can be found in all catchments. Especially in the period around day 241 in 1988/89 can be noted. The simulated runoff values are too low for all three catchments, probably due to error in the modelling of snow cover. This is also re¯ected in the period after day 301 where the simulated runoff values are all too high. It is also interesting to note the differences between the catchments. For example, the ¯ow peak between day 61 and 121 in 1986/87 is wrongly simulated in all three catchments. In FyrisaÊn it is too low, in LillaÊn it is a 266 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 Table 2 Model performance efficiency (R2) for the gauged river basins in the NOPEX areaa Year Basin FyrisaÊn SagaÊn LillaÊn È rsunO daaÊn HagaaÊn SaÈvaaÊn SaÈvja-aÊn StalbobaÈcken StabbybaÈcken Total gauged area 1981/82 1982/83 1983/84 1984/85 1985/86 1986/87 1987/88 1988/89 1989/90 1990/91 1991/92 1992/93 1993/94 1994/95 0.73/0.76 0.81/0.84 0.72/0.78 0.78/0.84 0.83/0.88 0.88/0.94 0.86/0.91 0.70/0.84 0.91/0.93 0.77/0.92 0.80/0.87 0.90/0.94 0.70/0.87 0.72/0.78 0.60/0.64 0.56/0.60 0.57/0.61 0.83/0.86 0.50/0.28 0.48/0.46 0.48/0.51 0.25/0.33 0.69/0.76 0.35/0.19 ± ± ± ± 0.72/0.72 0.62/0.70 0.65/0.81 0.75/0.90 0.69/0.74 0.57/0.71 0.72/0.85 0.32/0.46 0.66/0.77 0.62/0.84 0.60/0.77 0.74/0.78 0.40/0.76 0.61/0.78 0.83/0.88 0.52/0.73 0.64/0.72 0.84/0.94 0.80/0.81 0.69/0.72 0.76/0.85 0.22/0.60 0.77/0.85 0.62/0.74 0.52/0.70 0.71/0.73 0.39/0.71 0.53/0.91 0.64/0.75 0.43/0.83 0.56/0.82 0.77/0.96 0.76/0.81 0.53/0.71 0.56/0.66 0.26/0.64 0.70/0.92 0.53/0.62 0.19/0.44 0.64/0.78 0.59/0.74 0.24/0.70 0.76/0.83 0.62/0.80 0.69/0.75 0.90/0.96 0.82/0.91 0.73/0.84 0.75/0.80 0.27/0.64 0.80/0.89 0.71/0.78 0.57/0.80 0.65/0.72 0.55/0.75 0.69/0.91 0.65/0.73 0.53/0.61 0.50/0.63 0.82/0.93 0.86/0.90 0.69/0.77 0.66/0.77 0.19/0.58 0.83/0.88 0.60/0.65 0.63/0.77 0.78/0.85 0.61/0.80 0.69/0.84 0.14/0.29 0.70/0.72 0.84/0.83 0.75/0.88 0.30/0.20 0.45/0.54 0.75/0.83 0.62/0.76 0.85/0.90 0.60/0.68 0.57/0.58 0.73/0.79 0.46/0.50 0.67/0.66 0.58/0.72 0.59/0.60 0.61/0.66 0.68/0.93 0.57/0.81 0.54/0.75 0.57/0.77 0.26/0.44 0.75/0.91 0.71/0.85 0.44/0.70 0.76/0.85 0.54/0.75 0.65/0.95 0.79/0.81 0.76/0.80 0.74/0.78 0.90/0.95 0.88/0.90 0.77/0.79 0.77/0.83 0.48/0.68 0.86/0.90 0.72/0.75 0.81/0.91 0.84/0.87 0.67/0.88 0.80/0.92 1981±91 0.81/0.87 0.57/0.60 0.69/0.81 0.75/0.83 0.63/0.81 0.77/0.86 0.71/0.80 0.57/0.67 0.61/0.78 0.81/0.85 1981±95 0.81/0.87 ± 0.67/0.80 0.71/0.83 0.60/0.80 0.76/0.85 0.71/0.81 0.59/0.68 0.62/0.79 0.82/0.88 a Numerator: R2 day; Denominator: R2 month; 0.00: data included in calibration; 0.00: validation. bit too high and in StabbybaÈcken it is much too low. This shows that the parameterisation of the model does not manage to re¯ect all the differences between the catchments. Numerical experiments have shown that the calibration results could be improved slightly if the parameters of the model were calibrated separately for each basin. The parameter values were naturally different for different basins in this case. A good agreement between the observed and simulated values with the use of separately calibrated parameters does not guarantee that they can be assigned a physical meaning or that they will be transferable to other basins. A good model performance can be obtained for many different combinations of optimised parameters. It was easy to check that the parameters obtained for one basin did not provide a good performance of the model when applied in another basin. In the case where a global set of parameters have to be found for a number of basins with different conditions of ¯ow formation, the probability of ®nding the `correct' values, which can be reasonable in the physical sense, increases. This was proved by the results of simulations using the same parameters in other basins in the NOPEX area (see Table 2). Fig. 5 shows the observed and simulated discharge values for a few basins in the NOPEX area for 2 years: one with `satisfactory' agreement (with respect to R2) Ð 1986±87, and the other with `the worst' agreement Ð 1988±89. The visual impression is that the simulation results are not worse for the catchments used for validation than for those used for calibration. Here the same differences between the two years can be seen for the catchments used for validation as those used for calibration. Also here it is interesting to note the differences between the catchments. For example, the observed response for the event between day 61 and 121 is different in SaÈvjaaÊn than in all the other catchments. This is not re¯ected in the simulation results. It is also seen that StalbobaÈcken is the only catchment for which the simulations of the last days of 1988/89 are comparable to the observed runoff. As a summary these ®gures shows that the differences between the catchment are not totally accounted for in the model structure and that some years are more dif®cult to model than others and that the estimation of global parameters is possible. Sensitivity analysis has shown that the best model performance for separate basins was achieved when at least the one parameter Ð horizontal hydraulic con- Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 267 Fig. 5. Validation of the model performance; comparing observed and modelled runoff at independent basins not used in the calibration of regional parameters. ductivity of the soil, which de®nes the rate of subsurface ¯ow, slightly differs from the `global' value for different river basin usually not more than two times. However for SagaÊn basin this difference was about ®ve times. According to common practice (e.g. Popov, 1979) simulation results are considered to be good for values of R2 0.75, while for values of R2 between 0.75 and 0.36 the simulation results are considered to be satis- factory. This would correspond to multiple correlation coef®cients of R 0.86 and 0.60, respectively, in a regression problem. In this gradation good simulation results, based on daily observations, were obtained for FyrisaÊn, SaÈvaaÊn and for the total gauged area of all the basins. For the rest of the basins the agreement was satisfactory. The values of R2 obtained as the average of monthly values were good for all the basins with the exception of SagaÊn and StalbobaÈcken, where 268 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 they were satisfactory. It should also be mentioned, however, that the gradation referred to is as a rule applied for individually calibrated basins, while in this study we are dealing with regional hydrological calculations with a global set of parameters for the whole NOPEX area. Experience will show what are reasonable accuracy demands for this more demanding situation. Comparing the diagrams in Figs. 4 and 5 it is also seen that the simulated curves are as a rule more peaked than the observed ones. This can be explained by the fact that at this stage the actual amount of water delivered to the river net from REA elements is calculated and the ¯ow transformation in the channel is not considered. For small and medium-sized basins with a lag time of less than the one day used in the simulations, this does not make any signi®cant difference. A consideration of the transformation in the channel would smooth the hydrographs and possibly increase the R2 for daily values in the case of larger basins. It should also be noted, that when hydrological and meteorological models are to be coupled, the instantaneous values of hydrological cycle characteristics are required and, in particular, the amount of water delivered to the river net. The agreement between the simulated and observed discharge at the outlet sites of river basins including channel transformation is of a secondary importance in this case. The R2 ef®ciency criterion re¯ects the agreement of observed and calculated hydrographs, i.e. the dynamics of discharge and to a less extent ¯ow volumes. Table 3 shows the results of a comparison of the simulated water balance characteristics with the observed values from Seibert (1994). It is seen that the precipitation values used in simulations and those de®ned by Seibert are different. This discrepancy is explained by the difference in the method of calculation of areally averaged precipitation for the basins. Seibert obtained the mean values of precipitation for the river basins by multiplying the values of precipitation at each gauging station by individual correction factors. In the ECOMAG model precipitation values for each basin were obtained by weighted averages of the observations at the nearest stations. A correction factor of 1.2 was used to compensate for loss of precipitation catch due turbulence for all the stations with precipitation less than 40 mm per day and 1.0 for higher daily precipitation. Calculation of areally averaged precipitation for the basins was done by means of interpolation of the observations to 2 km grid cells with the use of kriging. A comparison of the runoff values in Table 3 shows that the simulated values were unsatisfactory for SagaÊn. No obvious reasons for such a discrepancy were found as physiographic conditions of runoff formation in SagaÊn are similar to those for other river basins in the NOPEX area, in particular FyrisaÊn, for which the agreement was good. At the same time, the difference between the measured average annual values for FyrisaÊn and SagaÊn is 150 mm for evaporation and 124 mm for runoff. One of the possible reasons for the discrepancy may be the poor quality of the observed data, caused by inaccuracies in the rating curve. In any case, the observed data for SagaÊn need a thorough analysis to sort out this problem. Table 3 Annual water balance of the gauged river basins in the NOPEX area (1981±91) according to Seibert (1994): observed precipitation (P*), observed runoff (Q*) and evapotranspiration as residual term (E*); and according to ECOMAG modelling: observed precipitation (P), calculated evapotranspiration (E) and calculated runoff (Q). Q Qmodel ÿ Qobserved Basin Station P* (mm) E* (mm) Q* (mm) P (mm) E (mm) Q (mm) Q (mm) |Q/Q*| (%) FyrisaÊn SagaÊn LillaÊn È rsundaaÊn O HaÊgaaÊn SaÈvaaÊn SaÈvjaaÊn StalbobaÈcken StabbybaÈcken Ulva Kvarn SoÈrsaÈtra GraÈnvad HaÈrnevi Lurbo Ransta SaÈvja TaÈrnsjoÈ Stabby 755 729 726 738 750 734 732 733 639 534 384 481 448 436 456 488 462 458 222 346 245 290 313 278 245 272 235 731 720 709 715 716 715 719 728 709 502 484 461 468 450 464 464 472 463 229 237 249 248 265 251 254 257 246 7 ÿ109 4 ÿ42 ÿ48 ÿ27 9 ÿ15 11 3 31 2 14 15 10 4 6 5 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 Fig. 6. Validation of the model performance; (a) synoptic runoff observations at 12 sites in the Fyris river and (b) comparison with those modelled from four different campaigns. 269 270 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 6.2. Synoptic runoff measurements An impression of the spatial variability of river runoff can be obtained through synoptic runoff measurements (Krasovskaia, 1988). Four surveys of runoff were performed in the FyrisaÊn river basin at 38 sites during ¯ow recession, two for wet conditions and two for dry conditions. It was possible to identify 12 of these sites along the river network used in the model (Fig. 6a). Fig. 6b shows a comparison of the simulated and measured river runoff for these 12 sites on the four occasions. In general the agreement is good especially when considering that the synoptic data have not at all been involved in the calibration. The range of variation and the variance are not signi®cantly different for both datasets. The discrepancies that appear in a more detailed analysis cannot at present be fully explained. The main reason is probably due to inaccuracy in determination of the areas of small tributaries and the spatial interpolation of meteorological characteristics, especially rainfall. Besides, it should be noted that the synoptic runoff measurements, describing instantaneous discharge values, were carried out over 2 or 3 days. The modelled discharges, on the other hand, give the average for a certain day. This might also cause discrepancies. 6.3. Soil moisture content and groundwater levels Soil moisture content and groundwater levels were observed in a number of small experimental basins within the NOPEX area during CFE1 and CFE2 (the measurements were performed also outside CFEs periods). The observation points were chosen to represent different geomorphologic units (hollow, slope and nose), soil types (till, clay, sand) and land use (open area, forest, mire) found in the area. Simultaneous campaign measurements were performed in these experimental basins. The data obtained within each such basin were averaged and taken as a characteristic of an assumed REA. These data were used for the adjustment of soil water parameters at the stage of model calibration. Table 4 offers information about the number of observation points in each basin including their soil and land surface cover type. Table 5 gives information of the model performance for soil moisture and groundwater levels in terms of the R2 ef®ciency measure and Fig. 7 allows a Table 4 Number of observation points of soil moisture and groundwater levels within experimental drainage basins Basin Number of observation points Soil type Land use Soil moisture Groundwater Buddby 151 DansarhaÈllarna 75 È stfora O 50 Marsta 25 TaÈrnsjoÈ 50 16 16 19 ± ± till till till/sand clay sand forest forest forest open area forest comparison of observed and simulated values of these variables. The modelled and averaged observed soil moisture contents are in general in good agreement. R2 is greater than 0.83 for four of the sites. TaÈrnsjoÈ has the poorest agreement, which can be explained by the small variance in the observed values. The ®gure shows that there is only one observation in the relatively wet period in springtime. TaÈrnsjoÈ is also very special for the NOPEX-area, placed at the top of an esker. It can be noted, that soil moisture measurements were carried out in the top soil layer, 15±20 cm thick on average, while soil moisture content has been modelled for an averaged 40±60 cm thick soil layer (horizon A). This difference might contribute to making the observed soil moisture content much more sensitive to external factors (rain, evaporation) than the more integrated modelled results, causing discrepancies between the curves. The modelled values of groundwater levels also follow well the averaged values of the groundwater level measurements. R2 is greater than 0.48 for all sites. The agreement is, however, not as good as for the soil moisture content. This is mainly explained by the Table 5 The model performance for soil moisture and groundwater levels in terms of the R2 efficiency measure Experimental catchment R2 soil moisture R2 groundwater Buddby DansarhaÈllarna Marsta È stfora O TaÈrnsjoÈ 0.87 0.83 0.84 0.83 0.42 0.55 0.52 ± 0.48 ± Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 271 Fig. 7. Comparing observed and modelled soil moisture content at five experimental basins and observed and modelled groundwater levels at three experimental basins (Each cross represents a spatial average, compare Table 4). 272 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 fact that the groundwater observation tubes did not represent the variability in a REA well enough, partly due to technical problems of installation of groundwater tubes in till soil. In particular, groundwater tubes in nose positions went dry during longer periods without rain. This fact in¯uences the calculated averages so that they are systematically underestimating the average groundwater depth. The modelled groundwater depth is accordingly deeper than the observed averages for till soils during dry conditions. 6.4. Vertical flux exchange and water balance The NOPEX concentrated ®eld efforts during May± June 1994 and April±July 1995 provide high quality datasets for estimation of vertical ¯uxes, especially evapotranspiration (latent heat ¯ux). Measurements were performed at a range of scales, in time and space, on the ground and from airborne and space platforms. In many contexts these different ¯ux estimates are not directly comparable due to differences in temporal and spatial scales. Local measurements from masts allow calculation of `point' estimates of heat ¯uxes from lakes and land surfaces (forest, mires, and agricultural land) using eddy correlation, pro®le and sap ¯ow methods. During events with airborne and radiosounding measurements, estimates of the ¯uxes are also available along ¯ight transects. Regional ¯ux estimates of sensible and latent heat for the whole and/or parts of the area are available from meso-scale climate modelling. A systematic evaluation and critical comparison of the different estimates including those of the ECOMAG model have been performed (Gottschalk et al., 1999). The analysis of data within the NOPEX project is in an early stage and the methodological problem of comparison of different ¯ux estimates has been stressed in this comparison. Table 6 shows components of the water balance estimated with ECOMAG for CFE1 and CFE2. The calculations show that during CFE1 the modelled evaporation was 10 mm higher than the observed precipitation and the runoff was as low as 6 mm. During the longer CFE2 period the evaporation and runoff part of the water balance was 156 mm higher than the precipitation. This difference between precipitation on one hand and evaporation and runoff on the other during both CFE periods is balanced by a decrease of the soil moisture and groundwater supply, Table 6 Water balance of the NOPEX area during periods CFE1 and CFE2 according to ECOMAG Period Precipitation Evaporation (mm) (mm) Runoff (mm) Wa (mm) CFE1 27 May± 23 June 1994 CFE2 18 April± 14 July 1995 64 74 6 ÿ16 215 289 82 ÿ156 a W: Water supply changes in soil and groundwater zone. accumulated during snowmelt and rain in winter and spring. Fig. 8a and b illustrate the patterns of the main hydrologic elements for CFE1 and CFE2 periods, respectively. The components show relatively large variation across space. The smoothest variation is revealed by precipitation, which is partly explained by the method used for interpolation here (kriging). An evaluation of precipitation from weather radar data gives a more patchy result (Crochet, 1999). It is seen that during both periods the lowest precipitation amount is found in the southwestern part of the NOPEX area, while the highest values are observed in the northern part for CFE1 and northeastern part for CFE2. The full daily data sets of all water balance components for CFE1 and CFE2 are provided in Gottschalk et al. (1999). As far as evaporation is concerned, the highest values during both periods were observed in the north-eastern part covered by forest on primarily till soils, while the lowest evaporation values are found in the south-eastern part of the NOPEX area with mainly clay soils and shallow bedrock. At a more detailed resolution a decrease in evaporation values in the areas with sandy soils is observed, while the evaporation values increase over lakes and mires. The current version of the ECOMAG model does not consider the role of different vegetation characteristics for evapotranspiration. There are still obstacles, mainly related to scale issues, to overcome, in order to correctly compare ¯ux estimates with model calculations for individual `points', patches and fundamental units (REA). Preliminary comparisons with mainly mast measurements give good agreement for individual patches on a daily base, although some discrepancies are noted. The variability across space shown Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 273 Fig. 8. The calculated water balance of the whole NOPEX area for (a) CFE1 (27 May±23 June 1994) and (b) CFE2 (18 April±14 July 1995). The size of the pixels are 2 km 2 km. by the model remains to be supported by independent measurements. Runoff patterns during CFE1 and CFE2 are nonhomogeneous due to the nonlinearity of the runoff formation process involving factors such as precipitation, soil and land-use patterns, slopes etc. In general, the highest speci®c runoff values are found in areas with shallow bedrock and sandy soil. These soils have low water storage capacity in the unsaturated zone and, as a rule, moderate evaporation, active recharge of groundwater and high base ¯ow and occur in association with eskers and in areas with steep slopes. Low runoff values during the relatively short periods of CFE1 and CFE2 are found in areas with peat and mires, though in the context of a longer time period (e.g. a year) the simulation shows that mires act as runoff regulators. Low runoff was also found in ¯at areas. Table 7 shows the values of the simulated and measured river runoff in the gauged basins of the NOPEX area for the CFE1 and CFE2. It is seen, that in general, the results are in a good agreement for the runoff (with the exception of LillaÊn) and also for the maximum daily discharges. 274 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 Fig. 8 (Continued ) Soil moisture distribution patterns are in general more directly related to the soil type. Higher soil moisture content is found in areas with peat and clay soils, while soil moisture content is low in areas with sandy soil and shallow bedrock. The main comparison is performed for regional ¯ux estimates for the whole NOPEX area (Gottschalk et al., 1999). The comparisons have been made for individual days when all different estimates were available as well as for the whole of CFE1 and CFE2 when only mast measurements and estimates from the meso-scale meteorological model and the ECOMAG model were available. The agreement is acceptable taking into consideration the uncertainty of the different estimates, but the problem needs further investigations. The regional estimates of evapotranspiration by a weighted average of mast measurements for CFE1 are 67 mm and CFE2 335 mm. The corresponding estimates by the ECOMAG model are 74 and 289 mm, respectively. 7. Conclusions A physically-based distributed hydrological model ECOMAG has been applied to nine river basins within Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 the NOPEX area with the purpose of validating its ability for regional modelling i.e. a repeated use of the model everywhere within a region with a global set of parameters. The NOPEX concentrated ®eld efforts during 1994 (CFE1) and 1995 (CFE2) as well as the continuous climate and runoff monitoring provide high quality datasets for such a validation. Most parameters of the ECOMAG model have a physical interpretation, for example soil physical parameters, which can, in principle, be measured. Others can be given reasonable values from experience, for example the degree-day factor. However, calibration of some model parameters is required to achieve an acceptable model performance. The question put forward here is whether a calibration of a global set of parameters on a few basins in a region provides acceptable performance for basins not used in the calibration and for variables not included in the calibration procedure. Evidence cited herein supports this minimal calibration with some caveats. The global parameters were determined from a joint calibration against runoff data for seven years from three drainage basins with an additional adjustment of soil parameters against soil moisture and groundwater level data from ®ve small experimental sub-basins in 1994±95 including CFE periods. The model with these parameters was then validated against runoff data for 14 years from six other basins and the remaining seven years for the three basins used for calibration, and against synoptic runoff measurements on four occasions in the largest drainage basin FyrisaÊn during CFE1 and CFE2. Finally, regional estimates of daily evapotranspiration were compared with estimates from ¯ux measurements, to give an independent assessment of the water balance. The performance of simulated runoff was evaluated by the Nash±Sutcliffe ef®ciency measure. For the larger basins and for the NOPEX area as a whole the results were classed as good and for other basins as satisfactory. A striking result is the variation in the performance criteria between different years, which partly might be explained by shifts between stable and unstable winter climatic conditions. Some discrepancies in the model performance are suspected to be caused by poor quality in regular runoff data. However, the overall result must be considered to be good as the simulations were performed without calibration. 275 The ability of the ECOMAG model to simulate the variation of average soil moisture for grid 2 km 2 km as showed by this study is also good. The performance has been evaluated by the Nash± Sutcliffe ef®ciency measure comparing averaged observed values for grid cells with those simulated. The performance is equally good for till, clay and sandy soils. Averaged observed and simulated groundwater level data have been compared in the same manner, with slightly poorer results than in case of the soil moisture. A problem here has been to obtain representative average groundwater level values for grids, because of the dif®culties with installing access tubes to suf®cient depth in till soils. A more problematic question is the comparison of synoptic runoff observations with those simulated. This focuses attention on the model's ability to reproduce the spatial variation in runoff. The total variability across space as assessed by the 12 synoptic points has a similar pattern for observed and simulated values but the individual deviations between them are dif®cult to explain at present. It has therefore not been possible to really validate the process description and parameterisation of drainage from individual grid cells. The different simulated water balance components for grid cells show relatively high spatial variability and it has not been possible to con®rm this variability from independent observations. This problem needs to be studied further. When simulated water balance elements were integrated to the whole NOPEX area, independent estimates from vertical ¯ux measurements of regional evapotranspiration have been used for validation. The noted discrepancies are within the uncertainties of the estimated values. A further step here would be to develop a data assimilation scheme for the regional model taking advantage of all separate data sources, not only those traditionally used in modelling efforts by hydrologists. References Abbott, M.B., Bathurst, J.C., Cunge, J.A., O'Conell, P.E., Rasmussenm, J., 1986. An introduction to the European hydrological model `SHE'. Journal of Hydrology 87(1/2), 45± 59. Arnell, N.W., 1993. Data requirements for macroscale modelling of the hydrosphere. In: Macroscale Modelling of the Hydrosphere, 276 Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 Proc. Of the Yokohama Symp., vol. 214, July 1993, IAHS Publ., pp. 139±149. Beldring, S., Gottschalk, L., Seibert, J., Tallaksen, L., 1999. Distribution of soil moisture and groundwater levels in the patch and catchment scale. Agric. For. Meteorol. 98±99, 305± 324. BergstroÈm, S., 1976. Development and application of a conceptual runoff model for Scandinavian catchments. Swedish Meteorological and Hydrological Institute RHO Report 7, NorrkoÈping. Beven, K.J., Kirkby, M.J., 1979. A physically based, variable contributing are model of basin hydrology. Hydrological Sciences Journal 24(1), 43±69. Crochet, P., 1999. Radar assessment of rainfall for the NOPEX area. Department of Geophysics, University of Oslo. Institute Report Series no. 104. DuÈmenil, L., Todini, E., 1992 A rainfall-runoff scheme for use in the Hamburg climate model. In: O'Kane, J.P. (Ed.), Advances in Theoretical Hydrology. A tribute to James Dooge, Elsevier, Amsterdam, pp. 129±158. Erichsen, B., Beldring, S., Rohde, A., 1995. Mesoscale runoff variability in the NOPEX area. Annales Geophysicae, Part II, Supplement II to vol. 13 (abstract). Feddes, R.A., Bresler, E., Neuman, S.P., 1974. Field test of modified numerical model for water uptake by root systems. Water Resources Research 10(6), 1166±1206. Gottschalk, L., Askew, A., 1987. Hydrology and data acquisition. In: Hydrology 2000, vol. 171, IAHS Publ., pp. 79±90. Gottschalk, L., Batchvarova, E., Gryning, S.E., Lindroth, A., Melas, D., Motovilov, Yu., Frech, M., Heikinheimo, M., Samuelsson, P., Grelle, A., Persson, T., 1999. Scale aggregation Ð comparison of flux estimates from NOPEX. Agric For. Meteorol. 98±99, 103±119. Gottschalk, L., Beldring S., Motorilor, Y., Siebert, J., 1999. Modelling of hydrological processes in different scales. Agric. For. Meteorol, 98±99. Documented dataset on appended CD. Gottschalk, L., Gryning, S.E., Motovilov, Yu.G., Beldring, S., 1998. NOPEX modelling activities: towards a coupled hydrological and meteorological mesoscale model. In: Fifth Meeting of the BALTEX SSG, vol. 10, Riga, Latvia, April 1997, International BALTEX Sectreteriat Publication, pp. A33±A42. Halldin, S., Gottschalk, L., Van de Griend, A.A., Gryning, S.-E., Heikinheimo, M., HoÈgstrom, U., Jochum, A., Lundin, L.-C., 1995. Science plan for NOPEX. NOPEX Technical report No. 12, Institute of Earth Sciences, Uppsala University. Halldin, S., Gottschalk, L., Gryning, S.-E., Jochum, A., Lundin, L.C., Van de Griend, A.A., 1999. Energy, water and carbon exchange in boreal forest. NOPEX experiences. Agric. For. Meteorol. 98±99, 5±29. Klemes, V., 1985. Sensitivity of water-resources systems to climate variations. WCP Report 98, WMO, Geneva. Klemes, V., 1986. Operational testing of hydrological simulation models. Hydrological Sciences Journal 31(1), 13±24. Knudsen, J., Thomsen, A., Refsgaard, J.C., 1986. WATBAL: a semi-distributed physically based hydrological modelling system. Nordic Hydrology 17, 347±362. Korzun,V.I., 1978. (Ed.), World water balance and water resources of the Earth. UNESCO, Studies and Reports in Hydrology, vol. 25. Krasovskaia, I., 1988. A study of mesoscale runoff variability. Geografiska Annaler 70A, 191±201. Kuchment, L.S., Demidov, V.N., Motovilov, Yu.G., 1983. Formirovanie rechnogo stoka: fisiko-matematicheskie modeli (River runoff formation: physicaly based models). Nauka, Moscow (in Russian). Kuchment, L.S., Demidov, V.N., Motovilov, Yu.G., 1986. A physically based model of the formation of snowmelt and rainfall runoff. In: Modelling Snowmelt-Induced Processes, Proc. Budapest Symp., vol. 155, July 1986, IAHS Publ., pp. 27±36 Kuchment, L.S., Motovilov, Yu.G., Startseva, Z.P., 1989. Sensitivity of evapotranspiration and soil moisture to possible climatic change. In: Proc. Conf. on Climate and Water, vol. 1, Helsinki, pp. 236±251. Motovilov, Yu.G., A model of snow cover formation, A model of snow cover formation and snowmelt processes. In: Modelling Snowmelt-Induced Processes, Proc. Budapest Symp., vol. 155, July 1986, IAHS Publ., pp. 47±57. Motovilov, Yu.G., 1987. Modelling the effects of agrotechnical measures on spring runoff and water erosion. In: Large Scale Effects of Seasonal snow Cover, Proc. of the Vancouver Symp., vol. 166, August 1987, IAHS Publ., pp. 241±251. Motovilov, Yu.G., 1993. The modelling of snowcover formation and snowmelt. In: The Modelling of the Hydrological Cycle for River Basins. Results of Research on the International Geophysical Projects. Russ. Nat. Geoph. Comm. Moscow, pp. 27±42. Motovilov, Yu.G., Belokurov, A.S., 1997. Modelirovanie protsessov perenosa i transformatsii zagryaznenii v rechnom basseine dlya zadach ecologiceskogo monitoringa (Modelling of transfer processes and pollution transformation in river basins for ecological monitoring). Inst. Appl. Geophys. Publ. 81, 49±60. Motovilov, Yu.G., Gottschalk, L., Engeland, K., Belokurov, A., 1999. ECOMAG a regional model of the hydrological cycle. Application to the NOPEX area. Department of Geophysics, University of Oslo. Institute Report Series no. 105. Motovilov, Yu.G., Nazarov, N.A., 1991. Modelled estimates of changes in the water balance of forested northern river basins. In: Northern Hydrology: Selected Perspectives, Proc. North. Hydr. Symp., July 1990, Saskatoon, Saskatchewan, Canada, NHRI Symp., vol. 6, pp. 499±513. Nash, J.E., Sutcliffe, J.V., 1970. River flow forecasting through conceptual models Part I-A discussion of principles. Journal of Hydrology 10, 282±290. National Research Council, 1991. Opportunities in the Hydrological Sciences. National Academy Press, Washington, DC. Nyberg, L., 1995. Soil- and Groundwater Distribution, Flowpaths, and Transit Times in a Small Till Catchment. Acta Universitatis Upsaliensis, Uppsala, Sweden. Popov, E.G., 1979. Gidrologicheskie prognozy (Hydrological forecasts). Gidrometeoizdat, Leningrad (in Russian). Rodhe, A., Beldring, S., Erichsen, B., Gottschalk, L., Siebert, J., 1999. Spatial variability in runoff, soil moisture and groundwater levels and its relation to terrain parameters. Agric. For. Meteorol. 98±99. Documented dataset on appended CD. Y.G. Motovilov et al. / Agricultural and Forest Meteorology 98±99 (1999) 257±277 Rose, C.W., Parlange, J.Y., Sander, G.C., Campbell, S.Y., Barry, D.A., 1983. Kinematic flow approximation to runoff on a plane: an approximate analytic solution. Journal of Hydrology 62, 363±369. Rosenbrock, H.H., 1960. An automatic method for finding the greatest or least value of a function. Computer Journal 17(3), 175±184. Sausen, R., Schubert, S., DuÈmenil, D., 1994. A model of river runoff for use in coupled atmosphere-ocean models. Journal of Hydrology 155, 337±352. Seibert, P., 1994. Hydrological characteristics of the NOPEX research area. NOPEX Technical Report No 3, Institute of Earth Sciences, Uppsala University. StaÈhli, M., Hessel, K., Eriksson, J., Lindhal, A., 1996. Physical and chemical description of the soil at the NOPEX central tower site. NOPEX Technical Report No 16, Institute of Earth Sciences, Uppsala University. Sulebakk, J.R., 1997. Geomorphometric studies of different topographic regions. Analyses and applications from Norway and Sweden. Dr. Scient. thesis, Department of Geography, University of Oslo, Report no. 8, Oslo. Tallaksen, L., Goltschalk, L., Ericksen, B., Lystad, S., Olsen, F., Soelthun, N.R., 1999. Modelling hydrological response to 277 evapotranspiration losses from different types of land cover. Agric. For. Meteorol. 98±99. Documented dataset on appended CD. Thomas, G., Rowntree, P.R., 1992. The boreal forest and climate. Q. J. R. Meteorol. Soc. 118, 469±497. Vinogradov, Y.B., 1988. Matematicheskoe modelirovanie protsessov formirovanija stoka (Mathematical modelling of runoff formation processes), Gidrometeoizdat, Leningrad (in Russian). VoÈroÈsmarty, C.J., Moore, B., Grace, A.L., Gildea, M.P., Melillo, J.L., Peterson, B.J., Rastetter, E.B., Steudler, P.A., 1989. Continental scale models of water balance and fluvial transport: an application to South America. Global Biogeochemical Cycles 3, 241±265. VoÈroÈsmarty, C.J., Moore, B., 1991. Modelling basin-scale hydrology in support of physical climate and global geochemical studies: an example using the Zambezi River. Surveys in Geophysics 12, 271±311. Wood, E.F., Sivapalan, M., Beven, K.J., Band, L., 1988. Effects of spatial variability and scale with implications to hydrological modelling. Journal of Hydrology 102, 29±47. Wood, E.F., Sivapalan, M., Beven, K.J., 1990. Similarity and scale in catchment storm response. Rev. Geophys. 28, 1±18.