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Validation of the Integrated Biosphere Simulator over Canadian deciduous and coniferous boreal forest.. Delire, Christine; Price, David T.; El Maayar, Mustapha; Black, T. Andrew; Foley, Jonathan A.; Bessemoulin, Pierre 2001-07-31

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JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 106, NO. D13, PAGES 14,339-14,355, JULY 16, 2001 Validation of the Integrated Biosphere Simulator over Canadian deciduous and coniferous boreal forest stands Mustapha E1 Maayar,   David T. Price, 1 Christine Delire, 2 Jonathan A. Foley, 2 T. Andrew Black,   and Pierre Bessemoulin 4 Abstract. Data collected during the Boreal Ecosystem-Atmosphere Study (BOREAS) at four different forest stands were used to test surface energy and carbon fluxes simulated by the Integrated Biosphere Simulator (IBIS). These stands included deciduous and conifer species and were located in both the BOREAS northern and southern study areas. Two runs were made: one using the original IBIS model and the other using a version modified to consider an organic soil layer (OSL) covering the mineral soil surface. Results show that the inclusion of the OSL substantially improved the simulation of soil heat flux, as well as of temperature and moisture in the topmost soil layer. Simulations show that latent and sensible heat fluxes, and net ecosystem exchange of carbon, were not affected appreciably by the presence of a thin (10 cm or less) OSL covering the forest floor. With a thick (50 cm) OSL, however, simulation of latent heat flux and net ecosystem exchange of carbon was substantially improved. Consideration of the OSL in the model also led to better simulation of the onsets of soil thawing. Correct estimation of heat diffusion to deep soil through thick organic layers requires a parameterization that accounts for the state of the organic material decomposition. Simulations presented here also show the necessity for using detailed information on soil physical properties for better evaluation of model performance. 1. Introduction Characteristics of vegetated terrestrial surfaces influence weather, climate, and atmospheric composition through their effects on exchanges of radiation, heat, water, momentum, and carbon [Shukla and Mintz, 1982; Pielke et al., 1997; Hogg et al., 2000]. For the last three decades, considerable modeling effort has been invested in understanding these influences. During this time, land surface parameterization models developed pri- marily for implementation in Atmospheric General Circula- tion Models (AGCMs) have evolved from simple aerodynamic bulk transfer formulae and uniform prescriptions of surface parameters (e.g., albedo, aerodynamic roughness, soil mois- ture) [Manabe and Bryan, 1969; Schneider and Dickinson, 1974; Manabe and Wetheraid, 1987] to more realistic representations of terrestrial biophysical processes (e.g., SiB of Sellers et al. [1986] and CLASS of l/erseghy et al. [1993]). More recently, process-based biophysical models have also taken into account photosynthesis and plant water relations to provide a more internally consistent description of the coupled fluxes of en- ergy, water, and carbon (e.g., the revised land surface scheme  Natural Resources Canada, Canadian Forest Service, Edmonton, Alberta, Canada. 2Center for Sustainability and the Global Environment, Institute for Environmental Studies, University of Wisconsin-Madison, Madison, Wisconsin. 3Department of Agroecology, University of British Columbia, Van- couver, British Columbia, Canada. 4M t6o-France, Service Central d'Exploitation de la M6t6orologie, Toulouse, France. Copyright 2001 by the American Geophysical Union. Paper number 2001JD900155. 0148-0227/01/2001JD900155509.00 SiB2 of Sellers et al. [1996], the revised ISBA of Calvet et al. [1998], and Dynamic Global Vegetation Models (DGVMs) such as the Integrated Biosphere Simulator (IBIS) of Foley et al. [1996]). The formulations of such models are necessarily complex yet must include numerous approximations and assumptions (be- cause many of the processes are themselves complex and re- main poorly understood). For this reason, an international Project for Intercomparison of Land Surface Parameterization Schemes (PILPS) was initiated [Henderson-Sellers and Brown, 1992], in which different land surface parameterizations were compared with observed flux data. Results involving 23 land surface schemes were reported by Henderson-Sellers et al. [1996] and Chen et al. [1997]. As pointed out by Delire and Foley [1999], however, the PILPS study did not include data from any forested sites. It is now fairly clear that the circumpolar boreal forest (of North America, Scandinavia, and northern Asia) plays an im- portant (if not crucial) role in regulating atmospheric CO2 content by acting as a carbon sink [Tans et al., 1990; Gates, 1993; Ciais et al., 1995; Sellers et al., 1997]. It may yet prove to be just as important in controlling the global climate [e.g., Bonan et al., 1992; Foley et al., 1994; Pielke and Vidale, 1995; Hogg et al., 2000]. Consequently, it is of considerable interest whether biospheric models such as IBIS, designed as dynamic vegetation schemes for use in AGCMs, can reproduce ob- served fluxes in this particular region, in addition to the general importance of validating them for different forest ecosystems. In the study reported here, the performance of IBIS operating in a stand-alone mode was investigated for different forests types located within the Boreal Ecosystem Atmosphere Study (BOREAS) region [Sellers et al., 1997]. These forest sites, lo- cated both in the southern and the northern study areas (SSA and NSA, respectively), are known within the BOREAS liter- 14,339 14,340 EL MAAYAR ET AL.' VALIDATION OF IBIS P Tu Eiu ET = Tu+Eiu+T +Ei +Es CO  shortwave longwave radiation radiation Runoff latent sensible heat heat CO  snow melt ..... . O cm .......................... 25 so .nfiltration ................  00 cm ................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................. heat diffusion ...................   soil moisture ...... to deep soil 200...cm ................ ! '\"\"'  diffusion SOil aecomposlnon ..... ............................... '\"\"';,; ..................................................................................................................................................................................................................................................................................................................................................................................................................................... .... 4..o..o.... .m ............................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................................... Figure 1. Schematic illustration of the water balance, the carbon balance, and the energy balance calcula- tions performed by IBIS. The following terms of the terrestrial water and energy budgets are explicitly simulated' evapotranspiration (ET), which is the sum of transpiration (T, and T ), evaporation from the soil surface (Ex), evaporation of water intercepted by vegetation canopies (Ei, and Ei ); runoff, soil water infiltration, subsurface drainage; latent, sensible, and soil heat fluxes; upward shortwave and longwave radiation; net carbon assimilation; autotrophic (root) and heterotrophic (microbes) respiration. Precipitation (P' rain + snow), downward shortwave and longwave radiation, and atmospheric CO2 concentration are prescribed. The subscripts u and l refer to the upper and lower canopies, respectively. ature as the northern old black spruce (NOBS), southern old jack pine (SOJP), southern old-aspen (SOA), and southern young aspen (SYA) stands. Within the North American boreal, forest dominated by black spruce (Picea mariana (Mill.) B.S.P.) is most common [Larson, 1980], although aspen (Popu- lus tremuloides Michx.) is the dominant deciduous species. In the BOREAS region, jack pine (Pinus banksiana Lamb.) is the secondmost common coniferous species. The BOREAS data therefore provide an important basis for validating IBIS when applied to high-latitude forest ecosystems. Only when such studies have confirmed that the model is able to provide real- istic responses to present-day climate for a range of ecosystems will it be appropriate to use it to assess effects of possible climatic changes on forest processes and distribution. 2. Model Description Version 2.1 of IBIS [Kucharik et al., 2000] was used in this study. This model is hierarchically organized to allow for ex- plicit coupling among ecological, biophysical, and physiological processes operating at different timescales [Foley et al., 1996]. Heat, momentum, and water exchanges are computed using the LSX land surface scheme model of Pollard and Thompson [1995]. LSX borrows its main structure from the SiB [Sellers et al., 1986] and BATS [Dickinson et al., 1986] models, simulating two vegetation layers (corresponding to upper and lower can- opies), and six soil layers with horizon thicknesses of 0.1, 0.15, 0.25, 0.50, 1.0, and 2.0 m, respectively. IBIS simulates carbon exchange and stomatal regulation of both Cs and C4 plant species according to a semimechanistic approach based on physiological evidence [Farquhar et al., 1980; Ball et al., 1986; Collatz et al., 1991, 1992]. Net ecosystem exchange (NEE) is computed as the difference between carbon taken up by the vegetation through gross (canopy-level) photosynthesis and carbon lost through plant respiration of foliage, wood, and roots and through microbial decomposition of litter and soil organic matter. For all the simulations reported here, vegeta- tion was treated as \"static\" in the IBIS vegetation dynamics module; i.e., no change in stand structure was assumed to occur during the periods for which simulations were per- formed. Figure 1 provides a schematic description of the LSX land surface scheme as coupled with the photosynthetic model of Collatz et al. [1991] and the soil respiration model of Lloyd and Taylor [ 1994]. 3. Data and Study Sites Detailed descriptions of sites, instrumentation, and mea- surements are reported by Black and Nesic [1999] and Chen et al. [1999] for SOA; by Bessemoulin and Puech [1998] for SYA; by Baldocchi et al. [1997a, 1997b] for SOJP; and by Goulden et al. [1997] for NOBS. Measurements of turbulent fluxes of latent and sensible heat, and NEE were performed using the eddy correlation technique (referred to from here on as EC). EL MAAYAR ET AL.: VALIDATION OF IBIS 14,341 Table 1. Vegetation and Soil Parameters Used for the Simulations Forest Site SOA SYA SOJP NOBS Vegetation Parameters Vegetation type upper trees trees trees lower shrubs C3 grass Fractional vegetation cover upper 0.8 0.9 0.8 lower 0.8 0.8 Vegetation height, m upper 21.50 2.75 13.50 lower 2.00 0.20 Leaf area index (LAI) upper daily a 5.5 2.4 lower daily b 2.0 Stem area index (SAI) upper 0.4 0.4 0.2 Vmax c upper 30.0 30.0 25.0 lower 27.5 25.0 Soil Parameters Soil texture silty loam silty loam sand Soil sand/silt/clay content, 20/65/15 20/65/15 92/05/03 % Soil depth, m 1.00 1.00 1.00 Organic layer thickness, m 0.08 0.08 0.05 Initial soil temperature, øC 12.1/10.6/10.0/ 12.1/12.1/12.1/ 13.4/12.1/11.6/ (by layer) 9.3 12.1 11.6 Initial soil moisture content, 0.58/0.58/0.47/ 0.16/0.23/.23/ 0.1/0.1/0.1/ m3/m 3 (by layer) 0.37 0.38 0.15 Initial soil ice content, m3/ 0.00 0.00 0.00 m 3 Soil porosity, m3/m 3 mineral soil 0.50 0.50 0.44 organic soil 0.80 0.80 0.80 Field capacity, m3/m 3 mineral soil 0.33 0.33 0.09 organic soil 0.60 0.60 0.60 Wilting point, m3/m 3 mineral soil 0.13 0.13 0.03 organic soil 0.20 0.20 0.20 Saturated hydraulic mineral soil 0.25 0.48 1.46 conductivity, m/d organic soil 0.25 0.48 1.46 Saturated air entry mineral soil 0.21 0.21 0.07 potential, m organic soil 0.21 0.21 0.07 Soil b parameter mineral soil 4.70 4.70 1.70 organic soil 4.70 4.70 1.70 Total soil carbon, kg-C/m 2 3.60 3.60 1.42 Total litter carbon, kg-C/m 2 1.11 1.11 0.67 trees 0.9 10.00 4.5 0.6 25.O silty clay 10/45/45 4.00 0.5 -5.9/-4.3/-3.5/ -2.0/-0.49/-0.5 0.0 0.0 0.80 0.48 0.80 0.39 0.60 0.25 0.20 0.46 0.46 0.34 0.34 7.90 7.90 4.18 0.48  'LAI ..... (upper canopy) is 2. bLAImax (lower canopy) is 2.3. CVma x is the maximum Rubisco capacity at 15øC of the top leaf. Their values were taken from Kucharik et al. [2000]. All observed data were recorded at half-hourly intervals. Only hourly data were used; however, data collected on the half hours were deleted except for precipitation where half hourly data were added to obtain hourly data (mm h-  ). Tests showed that no pertinent information was lost using hourly in place of half-hourly observations. The SOA site was an extensive 70-year old stand, dominated by aspen, located in the BOREAS Southern Study Area (SSA) at-- 53.7øN, 106.2øW. Average tree height was -- 21.5 m. The understory vegetation was composed mainly of hazelnut (Cory- lus comuta Marsh) -- 2 m tall. The soil is predominantly an Orthic Luvisol with an 8-10 cm deep surface organic layer [Black et al., 1996]. Data used in this study were collected during the 1996 field campaign and cover the period June 1 to December 31. The SYA site was also located in the SSA, with approximate coordinates of 53.39øN, 105.20øW. The stand was dominated by aspen, with very high stem density ( 10 stems m -2) and a mean tree height of 2.75 m. Soils ranged from gray wooded to degraded black, classified in the brunisolic, gleysolic, chernoz- emic, luvisolic, and organic soil orders. Data reported here were obtained in the period July 17 to August 16, 1994. No NEE measurements were available for this site. The SOJP site was located in the SSA region at 53.55øN, 104.41øW. Dominated by jack pine, with a mean canopy height of 13.5 m, the stand extended for over one kilometre from the instrument tower in all directions. Understory shrubs were sparse, consisting of isolated patches of alder (Alnus crispa). Ground cover was extensive however, including bearberry (Arctostaphylos uva-ursi), bog cranberry (Vaccinium vitis ideae), and lichens (Cladina spp.). Soil was a coarse textured sand, classified as a degraded Eutric Brunisol/Orthic Eutric Brunisol. Data used in this study were obtained for the period July 1 to September 16, 1994. The NOBS site was located in the BOREAS Northern Study Area (NSA) at 55.88øN, 98.48øW, surrounded by a black spruce-dominated forest of varying stature extending for sev- eral kilometers in all directions [Goulden et al., 1997]. Mean tree height was -- 10 m. Soils in this area consist of organics, clays, and some sandy deposits. Data used in this study were 14,342 EL MAAYAR ET AL.' VALIDATION OF IBIS 800 E 600 ,.  400 ,- 200   0 800 600 400 200 0 RB 0 200 400 600 800 Sn b 0 200 400 600 800 For the NOBS site, initial soil water content was assumed equal to porosity and all in the form of ice. Initial soil moisture content values at the SYA and SOJP sites were taken from Cuenca et al. [1997] and Nijssen et al. [1997], respectively. Soil textures for SOA and SOJP sites were classified as silty loam and sandy, respectively, based on data given by Cuenca et al. [1997] (Table 1). For the NOBS site, soil texture data were taken from the global data set used in large-scale simulations with IBIS [Foley et al., 1996]. Soil at the SYA site was assumed to have the same texture as that found at the SOA site. For all SSA sites, soil hydraulic properties were taken from Nijssen et al. [1997] and Cuenca et al. [1997], with soil depth set to 1 m, following data from Clayton et al. [1977]. Fractional vegetation cover and leaf area index (LAI) for SOJP and NOBS, and stem area index values, were taken from Kimball et al. [1997], Nijssen et al. [1997], and Gower et al. [1997], respectively. Leaf area index at SYA was assumed equal to that reported for SOA by Black et al. [1996] for the period of the simulation, as also reported by R. D. Pyles et al. (personal communication, 1999). Daily changes in LAI at SOA, as reported by Chen et al. [1999], were approximated using a third-order polynomial function. Root profiles were as given by Nijssen et al. [1997] for SOJP and NOBS and as given by Jackson et al. [1996] for SOA and SYA. Total soil carbon and total litter carbon values, were taken from Gower et al. [1997] and Steele et al. [1997]. 500 450 400 350 300 250 200 Lup i i i i i i i 200 250 300 350 400 450 500 Observed (W m -2) Observed and simulated: (a) net radiation (R,), Figure 2. (b) net shortwave radiation (Sn), and (c) upward longwave radiation (Lup) at old aspen site during the period June 1 to December 31 1996. obtained for the period April 1 to October 9, 1996. No soil heat flux measurements were available at this site. For each hourly time step, IBIS simulated the energy and C balances using the following forcing variables: air temperature, hourly total precipitation, wind speed, humidity, incoming short-wave and long-wave radiation, and surface air pressure. Incoming long-wave radiation, whenever missing, was esti- mated using the formula of Satterlund [1979]. Occasional data gaps were filled using mesonet station data [Shewchuk, 1997]. In addition, site-specific regression equations, derived from measured data, that expressed net radiation as a function of incoming shortwave radiation, were used to fill very occasional gaps in shortwave radiation time series. The data used to initialize the model are shown in Table 1. Soil temperature data were available for all sites. For the SOA site, measured soil moisture was used to initialize the model. 4. Comparison of Observed and Simulated Data Two series of simulations were performed for each forest stand. The first series was carried out using only mineral soil texture classes, as used in IBIS2.1 simulations at the global scale by Kucharik et al. [2000]. For much of the Canadian boreal forest zone, however, particularly those vegetation com- munities dominated by aspen and spruce, an organic layer covers the surface [Clayton et al., 1977]. Typically, this layer is deeper in the northern regions because decomposition rates are normally lower than in the warmer conditions farther south. Hence, for our second series of simulations, an organic soil layer was introduced into the model, with hickness fixed according to observations made by Black et al. [1996] for the SOA site, by Baldocchi et al. [1997a] for SOJP, and by Clayton et al. [1977] for NOBS (see Table 1). For the SYA site we used the same thickness as that reported for SOA. At the SOA, SYA, and SOJP sites, only the top layer of the six model layers was treated as organic, but at NOBS the top four layers were all treated as organic, replacing the corresponding mineral soil layers. Moreover, when presence of organic soil was simulated, surface albedo was set equal to 0.1 (i.e., it was treated as a moist dark soil as defined in Table 6.4 of Brutsaert [1982]). Mineral soil albedos were computed by the model as a function of sand, silt, and clay fractions following Dickinson et al. [1986]. Heat capacity of dry organic material (0.58 MJ m -3 K - ) and thermal conductivity (0.06 W m -  K - ) were taken from Guyot [1997]. Because of the lack of information on the par- tide size distribution (or degree of decomposition) of the or- ganic matter layers at the study sites, saturated hydraulic con- ductivity and the soil b parameter (i.e., the exponent for the Campbell moisture release equation [Campbell and Norman, 1998]) were assumed to be the same in both sets of simulations: i.e., with and without the simulated soil organic layer. Data for saturated hydraulic conductivities at each site were obtained from Cuenca [1997]. EL MAAYAR ET AL.: VALIDATION OF IBIS 14,343 500 400 300 200 1 oo o -100 -200 6OO 500 400 300 200 1 O0 o -lOO   H IBIS   IBIS+ _ ß .'. '- v' \" ' _L ' '    ' . . . . ' '., ;..--..- ,-.-.. __ : :,,.: I I I I I I I -200 -100 0 100 200 300 400 500 -200 -100 0 100 200 300 400 500 -100 0 100 200 300 400 500 600 -100 0 100 200 300 400 500 600 G leaf period only total period of simulation 200 e (leaf+leafless periods) f ß . ß 100  - '. '...V4:g t '-. '. . .. ' ..., :: \" ,.'..',.'.,......'..- '.. '. . .. ' .-.,....,- ,.:.-..,?\". :.- T :.. 1 .,...., =:.. ß -100 [ \"' ß IBIS IB IS+osl I I I I I I I I I I I I I I I I -20 -lo 0  0 20 30 40 -20 - 0 0  0 20 30 40 Observed (W m -2) Observed (W m -2) 10 0 -10 -20 -30 -40 - NEE IBIS - 1BIS+osl , .  _- .-_:_':' \"-7 \":\"   ß ':': ? ::'  \" ß '.. -40 -30 -20 - 10 0 10 20 -40 -30 -20 - 10 0 10 20 Observed (gmol-CO 2 m -2 s - ) Observed (gmol-CO 2 m -2 s - ) Figure 3. Simulated hourly above-canopy fluxes plotted against data observed at the old aspen site during the period June 1 to December 31, 1996. (a) Sensible heat flux assuming presence of mineral soil only, (b) mineral soil with surface organic layer. (c) Latent heat flux assuming presence of mineral soil only, (d) mineral soil with surface organic layer. (e) Soil heat flux during the period when trees are in leaf, (f) when trees are leafless. Dark dots indicate that the run assumed the presence of mineral soil only and light triangles indicates that the run assumed the presence of mineral soil with surface organic layer. (g) Net ecosystem exchange (NEE) assuming presence of mineral soil only, and (h) mineral soil with surface organic layer. Carbon flux (NEE) flux is positive toward the atmosphere. 14,344 EL MAAYAR ET AL.: VALIDATION OF IBIS 400 t observed a IBIS ß 300 200 - lOO o - lOO 500 400 300 200 100 50 -50 ' al 0 . *,  e e e e , [..T..  -30 t 0,,  ee  ''  Z; 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 Day of year Figure 4. Observed and simulated diurnal variation of: (a) sensible heat flux, (b) latent heat flux, (c) soil heat flux, and (d) net ecosystem exchange at old aspen site. Dots indicate assumed presence of mineral soil only; gray triangles indicate assumed presence of mineral soil with surface organic layer. Carbon flux (NEE) is positive toward the atmosphere. 5. Results 5.1. SOA Site Simulated and observed radiation and flux data are shown in Figures 2, 3, and 4. The agreement between observed and simulated net shortwave radiation (Sn) is high (Figure 2b), suggesting that the parameterization of surface albedo was fairly accurate. Agreement between observed and simulated fluxes of net radiation (Rn), and upward longwave radiation (Lup) is also reasonable, although R, is slightly underesti- EL MAAYAR ET AL.: VALIDATION OF IBIS 14,345 300 ........ observed _ a   IBIS (SAI=0.2) \" ! .... ': ': ..................................................... IBIS (SAI=0.4) \" :-   ' ß ! j \" i! IBIS (SAI=0.8) .. ß b :. -- c ... I I I I I I I I I I I I I I I 200 100 o -100 500 4OO 300 200 lOO o -100 1 oo ? 50 0 -50 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 Day of year Figure 5. Sensitivity of simulated energy fluxes to different input values of stem area index (SAI), at old aspen site: (a) sensible heat flux, (b) latent heat flux, and (c) soil heat flux. mated owing to overestimation of L up (Figure 2c). The latter results from overestimation of surface soil temperature (Fig- ures 5a and 5b). Agreement between observed and simulated latent heat flux (LE) (Figures 3c, 3d, and 4b) is higher than for sensible heat flux (H) (Figures 3a, 3b, and 4a) and soil heat flux (G) (Fig- ures 3e, 3f, and 4c). This bias obtained in the simulation of H causes a temporary imbalance, mainly around midday, in the total heat flux. Two other simulation studies reported a similar, but larger bias in the LSX model [Pollard and Thompson, 1995; Delire and Foley, 1999]. Analyzing the performance of LSX in tropical forests, Pollard and Thompson [1995] suggested that the heat imbalance was caused by exaggerated heat storage in trunks and stems (estimated from stem area index, SAT) and released mainly by evaporation during the night. To test this hypothesis, we ran the model for different values of stem area (Figure 5). Doubling the SAT increased the midday bias in both simulated sensible and latent heat fluxes, while halving the SAT led to a relative improvement in the simulation of LE as well as H (Figures 5a and 5b). Sensitivity of soil heat flux (G) to the selected value of SAI was relatively minor (Figure 5c). A fur- ther development of this point is pursued in section 5.3 where measured canopy heat storage data were available for the SOJP site. The model generally overestimates observed G (Figures 3e and 4c), a problem common to many land surface models, particularly when they are applied to forest sites [e.g., Shao and Henderson Sellers, 1996; Chen el al., 1997; Delire and Foley, 1999; Bellisario el al., 2000]. This evidently results from lack of consideration of the role of the organic layer usually covering forest floors. Indeed, after including an organic layer, referred to here as the IBIS + osl run (Figures 3e, 3f, and 4c), mean simulated G was much closer to the observed values, although it remained higher for daytime and lower for nighttime (Figure 4c). Poor numerical resolution of soil temperature near the surface is a common problem with land surface models, as explained by Bells el al. [1993] (working on surface parameter- izations for the European Centre for Medium-Range Weather Forecasts) and by Chen el al. [1997] (who carried out a PTLPS study involving 23 land surface schemes using data from the 14,346 EL MAAYAR ET AL.: VALIDATION OF IBIS Table 2. Averages and Standard Deviations of Observed and Simulated Fluxes a Standard Deviation Average Observed IBIS IBIS + osl Observed IBIS IBIS + osl nb of Observations SOA Forest-SSA Rn, W m -2 84.31 44.45 47.39 187.74 175.94 175.66 5039 H, W m -2 21.89 8.43 8.28 77.21 36.84 40.14 4632 LE, W m -2 48.11 53.28 55.00 82.22 93.89 102.93 4268 Bowen ratio, H/LE 0.46 0.16 0.15 0.94 0.39 0.39 4268 G, W m -2 0.82 -11.10 -9.53 6.51 40.00 25.41 4897 NEE-l,/ mol-CO 2 m -2 s -  -2.95 -3.70 -4.01 7.92 10.22 10.20 2591 NEE-2,/ mol-CO 2 m -2 s -  1.38 2.56 2.52 1.44 0.60 0.58 1672 NEE-3,/ mol-CO2 m -2 s -  -1.39 -1.45 -1.66 6.72 8.72 8.75 4263 SYA Forest-SSA Rn, W m -2 153.57 136.54 138.35 223.24 236.56 235.25 696 H, W m -2 13.81 29.12 29.21 49.46 39.49 41.41 676 LE, W m -2 94.48 100.92 104.05 116.49 107.71 121.36 666 Bowen ratio, H/LE 0.15 0.29 0.28 0.42 0.37 0.34 666 G, W m -2 2.44 6.41 5.07 15.07 40.31 19.91 696 SOJP Forest-SSA Rn, W m -2 121.73 88.03 87.84 194.63 204.71 200.33 1755 H, W m -2 61.32 52.08 56.85 110.59 85.98 92.16 1729 LE, W m -2 47.84 32.75 29.44 64.61 66.20 73.72 1722 Bowen ratio, H/LE 1.28 1.59 1.93 1.71 1.30 1.25 1722 G, W m -2 -1.40 2.14 1.51 18.20 33.62 14.79 1765 NEE,/xmol-CO 2 m -2 s -  -0.43 -0.40 -0.78 4.59 1.68 1.93 1716 NOBS Forest-NSA Rn, W m -2 124.03 87.09 87.23 202.93 216.25 215.58 4607 H, W m -2 63.13 50.54 50.33 126.05 84.63 85.79 4344 LE, W m -2 31.42 26.23 30.03 47.38 34.32 44.91 4322 Bowen ratio, H/LE 2.01 1.93 1.68 2.66 2.47 1.91 4322 G, W m -2 7.60 4.09 31.40 14.90 NEE,/ mol-CO 2 m -2 s -  -0.45 0.21 -0.57 3.03 1.16 1.44 4350 aIBIS + osl indicates that the first soil layer in IBIS was considered as organic for YA, OA, and OJP sites. Idem for OBS site but the four first soil layers was set as organic in this case. NEE-1 is the NEE for the period when trees are in leaf; NEE-2 is the NEE for the period when trees are leafless; and NEE-3 is the total NEE (NEE1 + NEE2). Depth of the soil organic layer used in the IBIS + osl simulation is: 8 cm for SOA and SYA, 5 cm for SOJP, and 50 cm for NOBS. Cabauw grassland site). This causes an amplification of soil heat fluxes and a delay of turbulent fluxes. Simulated and observed NEE data are shown in Figures 3g, 3h, and 4d. We adopted the convention that NEE is positive when the net flux is toward the atmosphere. Agreement be- tween the simulation and measurements is lower around noon then at other times of day. Delire and Foley [1999] reported a similar problem when comparing results of their simulation for a grassland site with data from the FIFE experiment [Verma et al., 1992]. Figure 4d also shows that the model generally over- estimates nighttime respiration. Recent analyses by BaMocchi et al. [1998] and Lee [1998] on the reliability of EC measure- ments of carbon exchange between the surface and the atmo- sphere in forests may help to explain these results. By analyzing the conservation equation of CO2 [BaMocchi et al., 1998, Equa- tion (1)]. These authors suggest that the conventional analysis of EC data may neglect an important advective effect in forests under stable conditions, occurring particularly at night. Al- though there is some controversy surrounding Lee's explana- tion, it is evident that the flux of CO2 from the air column below the instrument may be underestimated and hence mea- sured NEE is overestimated. Hence the model's slight under- estimates of observed nighttime NEE seen in Figure 4d may be reasonable. Conversely, the model evidently overestimates daytime NEE, which implies either that ecosystem respiration is underestimated or that net photosynthesis is also exagger- ated. The simulation of net photosynthesis is derived from the Farquhar-Collatz model, however, which assumes simulta- neous stomatal regulation of CO2 exchange and transpiration. The strong agreement between measured and modeled LE indicates that the photosynthetic flux is approximately correct, which therefore suggests more investigation of respiration pro- cesses within IBIS is warranted. Another source of the nighttime respiration discrepancy could originate from the soil carbon density data reported by Gower et al. [1997], that were used to initialize the model, and which affect soil respiration. These data (see Table 5 of Gower et al. [1997]), are considerably lower than those reported by other investigators (e.g., T. Nerbus and D. Anderson, Univer- sity of Saskatchewan, unpublished data, 1996; H. Veldius, Uni- versity of Manitoba, unpublished data, 1996). A higher value of initial soil carbon content would result in greater simulated soil respiratory fluxes during the growing season, assuming all other factors are unchanged. A sensitivity test showed, how- ever, that even if the higher value of initial soil carbon was used, it could not provide a complete explanation for the dis- crepancy obtained between measured and simulated midday NEE. Over the entire simulation period (NEE-3 in Table 2), the model explained ---96% of NEE measured at SOA (original IBIS run). This overall agreement hides fairly serious discrep- ancies, however, in both summer and winter data sets. For the EL MAAY  ET AL.: VALIDATION OF IBIS 14,347 30 15 -15 30 15 0 15 - 15 10 5 0- 150 i i i i _ _ a IBIS '  .............. IBIS+osl _ 8-25 cm - _ _ _ k__r   _ I I I 200 I 250 300 350 Day of year 24 16 12 8 l0 0 2O? - b soil 0-8 cm- 211 215 219 223 227 Day of year ' t 0.8 C ' 0-8 cm I - ...':...............: .... . ..... .........::  2 - 0cm t I I - 50-100 cm - 0.2 1,[ ..... , ..... i. . _,.,.. ,: ! i 153 200 247 Day of year Figure 6. Observed and simulated: (a) daily soil temperature, (b) hourly soil and stem temperatures, and (c) daily soil moisture content, at old aspen site. Note that the horizontal scales differ significantly between Figures 6a, 6b, and 6c. 0.6 0.4 0.2 0.4 0.2 0.5 0.4 0.3 _ 10.. o 5   0   period when trees are in leaf and NEE indicates net carbon uptake (NEE-1 in Table 2), the ratio of observed to modeled NEE is -0.81, compared to -0.54 for the period when trees are leafless and NEE indicates net carbon release (NEE-2 in Table 2). Simulated wintertime CO 2 effiux is generally much higher than it should be, suggesting that the temperature re- sponse of the soil respiration model is too shallow. While including the OSL substantially improved the simu- 14,348 EL MAAYAR ET AL.: VALIDATION OF IBIS lation of G, turbulent fluxes (H and LE) were virtually un- changed (Figures 3a-3d, 4a, 4b, and Table 2). Average NEE increased by -10% in response to the simulated OSL, al- though this response was restricted almost entirely to the grow- ing season (Table 2). The explanation for this appears to be that the organic layer increased water infiltration and reduced runoff, thereby increasing soil surface water availability (Fig- ure 6c) and reducing vegetation drought stress. This in turn led to a reduction in the seasonal constraints on vegetation- atmosphere exchanges of water and carbon. The model was able to reproduce stem temperature success- fully (Figure 6b), whereas soil temperature was generally over- estimated, but particularly in the topmost soil layer. This was due partly to the inconsistencies in the numerical solution of skin temperature mentioned previously. Adding the OSL to the original model resulted in greater soil moisture content in the top soil layer, however, which led to increased heat capacity and decreased soil surface soil temperature (Figures 6a and 6b). It should be borne in mind, however, that the results obtained from the IBIS + osl run are dependent on the value estimated for the saturated hydraulic conductivity of the or- ganic layer (see section 4). Moreover, the observations did not show any significant soil moisture increase in response to the high rainfall (-60 mm) recorded on Julian days 188 and 189 (Figure 6c), which suggests a problem in data acquisition dur- ing this period. Temperature of the 50-100 cm soil layer was also overesti- mated by the simulation between days 250 and 350. This sug- gests poor representation of heat diffusion to deep soil after the latter reached its peak temperature in the summer. 5.2. SYA Site Reasonable agreement between simulated and observed fluxes of R  and LE was obtained, although R  was slightly underestimated during nighttime (Figures 7a, 7b, 7e, and 7f). In general, H was overestimated, but particularly at night (Fig- ures 7c and 7d; see also Table 2). This nighttime exaggeration could be due to simulated release of heat stored in the canopy during the day. Daily stored energy is also likely to be partly released in the form of evaporation of water at night (Figure 7f). These nighttime releases would then cause, in turn, a systematic underestimation of nighttime R  for the SYA site (Figure 7b) as well for the other sites (Table 2). Figure 7d also shows that the diurnal course of simulated H generally lagged the observational data. As reported above, this originates from the delayed transfer of soil temperature information into the atmospheric boundary layer calculations. Nevertheless, as with the SOA site, simulating an organic surface layer caused a significant improvement in modeled soil heat flux, both tight- ening the distribution of points and shifting the regression slope closer to the 1:1 line (Figures 7g and 7h). 5.3. SOJP Site R  was simulated correctly during the day but underesti- mated at night (Figures 7a and 7b; diurnal cycle is not shown (see section 5.2. for illustration)). As for the deciduous forest sites (SOA and SYA), LE was generally better simulated than H (Figures 8c-8f). The disagreement between observed and simulated H around midday was smaller, however, than at the deciduous forest sites. The existence of measured data on canopy heat storage for this site allows verification of the explanation given in section 5.1 concerning underestimation of midday H by the model. Figure 9 shows clearly that when energy received by the surface was close to maximum, the simulated canopy heat storage could exceed 100 W m -2. Con- versely, during the night the model simulated greater release of stored energy than observed (Figure 9), causing H to be over- estimated (Figures 8c and 8d). Introducing the OSL produced no significant improvement in simulated H and LE fluxes, although G was substantially improved and to a greater extent than at the deciduous sites (Figures 8g and 8h). The largest discrepancy between measured and simulated NEE was also obtained around midday (Figures 8i and 8j; diurnal cycle not shown). Nighttime respiration was correctly simulated, however, which supports the hypothesis that the simulation of temperature effects on canopy respiration, dur- ing daylight periods in both coniferous and deciduous ecosys- tems, requires further modelling effort. Soil temperature was generally exaggerated by the model at this site (Figure 10). Furthermore, the discrepancy between observed and simulated soil temperatures increased with depth, suggesting that soil thermal diffusivity was significantly lower in reality than implied by the values used in the model. This conclusion was confirmed by simulating the OSL, which improved agreement for the upper soil layers (depths to 25 cm), but still resulted in appreciable overestimation of average temperatures. 5.4. NOBS Site In the northern boreal region, soil organic layers are typi- cally deeper than 50 cm [Clayton et al., 1977]. Hence, for the NOBS site located in the BOREAS-NSA, thickness of the OSL was set to 50 cm for the IBIS + osl run, corresponding to the top three soil layers in IBIS. Porosity, field capacity, and wilting point data (in terms of volumetric water content) were taken from Nijssen et al. [1997] (Table 1). The standard IBIS run, i.e., assuming only mineral soil at the surface was carried out using a silty clay soil texture, corresponding to that used in IBIS for global simulations (see section 3). As with the other sites, observed R  was simulated better for daytime than nighttime (Figures 11a and 11b). Including the organic layer resulted in almost no changes in simulated H (Figures 1 lc and 1 ld), but produced significantly better pre- diction of LE (Figures 11e and 11f). The major contributing factor for the improvement in LE was the reduction of G (Table 2; note that measurements of G were not available for this site), which resulted from the greater moisture storage capacity in the 50 cm OSL, compared to the lower porosity of the mineral layers. Comparison of observed and simulated mean Bowen ratios for this site and for OJP shows that both are greater than 1.0 (Table 2), whereas those for the deciduous sites were typically much lower. According to the Collatz [1991, 1992] model used in IBIS, changes in stomatal conductance to water vapour lead directly to changes in COx uptake. The improvements in LE resulting from including the OSL in the NOBS simulations therefore also appear to contribute to improved simulation of NEE, with both a higher mean and a wider range between minimum and maximum values (Figures 11g and 11h). As with the SOA and SOJP sites, however, NEE values around midday were over- estimated. When integrated over the whole period, the total simulated NEE indicates a slight carbon source when no or- ganic layer is included (Table 2), compared to an observed net sink for the measurement period. In the IBIS + osl simulation, EL MAAYAR ET AL.' VALIDATION OF IBIS 14,349 800   600   400 ,-  200 , ,  r  o RB 0 200 400 600 800 b 800 600 400 200 0 204 205 206 207 208 209 210 211 _ H i d 200 oo_ . o ø {o -100 I I I I I I I i I i 100 -100 0 100 200 204 205 206 207 208 209 210 211 5oo   5oo - LE   ..   :1' f - 400 300 - ß   . .'-'wM.y ;;': . ß .. 200- . 1 O0  Y J.'  '   .    .   10 -100  l i i i i i i I i i i i i - -100 -100 0 100 200 300 400 SO0 204 20S 206 207 208 209 210 211 120 ? 80 B: 40 '  0   -40 -80 G 120 80 40 -40 - I I I i I I - I I I i I I i I - -80 -40 -20 0 20 40 60 204 205 206 207 208 209 210 211 Observed (W m -2) Day of year Figure 7. Simulated hourly above-canopy fluxes plotted against data observed at the young aspen site during the period July 17 to August 16, 1994. (a, b) Net radiation. (c, d) Sensible heat flux. (e, f) Latent heat flux. (g, h) Soil heat flux. Dark dots indicate assumed presence of mineral soil only; light triangles indicate assumed presence of mineral soil with surface organic layer. however, the inclusion of an organic layer resulted in an aver- age net sink, comparable in magnitude to the observed value. Agreement between observed and simulated soil tempera- tures for the top layer also improved when the OSL was con- sidered (Figure 12), but with increasing depth, this agreement became progressively poorer. Inclusion of the OSL also im- proved the timing of the onset of soil thawing at the topmost layer. 14,350 EL MAAYAR ET AL.: VALIDATION OF IBIS 800 600 400 2oo o - Rn IBIS IBIS+osl - 0 200 400 600 800 0 200 400 600 800 . , 600 ,7, 400   200 m o r.  -200 - H IBIS . . . - IBIS+osl . ß . - C . ,, e..,-,.:..,j :. -.   - d _ I I I I I I I I I I I I I I - 100 0 100 200 300 400 500 - 100 0 100 200 300 400 500 , , 600 ?   400 ,-  200 -  o  .  -200 - ß ' ß IBIS -- LE ß _ ß ...,t øß .' ß ß :-...: . ' ' ,. '. .  ....-.,,;.,. -. _ I I I I I I - 100 0 100 200 300 400 . IBIS+osl - _ I I I I I I -100 0 100 200 300 400 150 lOO 50   o 15 lO 5 o -5 -15 -2o - G 1BIS - 1BIS+osl - ß ' 4, ,:_.'..i,. .: .'_. co ß ß  ,\" ',  =. ,  ,- ..  - .._. ..  - .-. ¾.:. ß ß . g ß h - m _ ' ' ' \"0 4'0 6'0' ' ' ' ' -40 -20 0 2 -40 -20 0 40 60 Observed (W m -2) Observed (W m -2)  NEE IBi     IBIS+ osl   .  _ ß ....a:.-. .:>', : .7 :. -- .  : .,,, .< ,: ...v  .' . - - ' \".: ,' :'.',..1tlI11 ,. '-.\"..\"' ..:.\". '.': ß + _ ß ..4:'.?,'7'_.\" '.?' .::'-:\"' ñ : \".: :'\"'\" '   ',,'\"  \";\"  .: ' - - :' ' \" \" ' ' i - \" ' ..... \"::\" \"': ' j - ..... i,: ' :- I -20 -15 -10 -5 0 5 10 15 -20 -15 -10 -5 0 5 10 15 Observed (gmol-CO 2 m -2 s -1) Observed (gmol-CO2 m -  s -1) Figure 8. Simulated hourly above-canopy fluxes plotted against data observed at the old jack pine site during the period July 1 to September 16, 1994. (a) Net radiation assuming presence of mineral soil only, (b) mineral soil with surface organic layer. (c) Sensible heat flux assuming presence of mineral soil only, (d) mineral soil with surface organic layer. (e) Latent heat flux assuming presence of mineral soil only, (f) mineral soil with surface organic layer. (g) Soil heat flux assuming presence of mineral soil only, (h) mineral soil with surface organic layer. (i) Net ecosystem exchange (NEE) assuming presence of mineral soil only, (j) mineral soil with surface organic layer. Carbon flux (NEE) is positive toward the atmosphere. 6. Discussion and Conclusions Collective understanding of the physical, physiological, and ecological processes governing terrestrial biospheric behavior has increased significantly over the last 30 years. As this un- derstanding has developed, so too has the desire to encapsu- late it in simulation models of increasing complexity. Current- generation biospheric models such as IBIS are highly EL MAAYAR ET AL.' VALIDATION OF IBIS 14,351 250 200 150 100 50 0 -50 -100 1 217 ..... observed IBIS 218 219 220 221 222 223 224 225 226 227 Day of year Figure 9. Illustration of diurnal variation of observed (dotted line) and simulated (original IBIS; solid line) canopy heat storage at old jack pine site during summer. sophisticated, but this sophistication also makes them very difficult to test. In order to have confidence in such models, e.g., when using them to investigate effects of future environ- mental changes on the biosphere, it is essential to test and validate them against observed data at the local (site-level) scale as well as at the continental and global scales. Hence, as a part of a project to explore climate change effects on Cana- da's forests, this study compared IBIS version 2.1 with data 25 20 15 10 20 15 10 ........ observed 0-5 cm IBIS ........................... IBIS+osl ,, /  t  ', \ ' ',   I'. ', , ,   '  \ .. .. _ _ i i i i i 5-15 cm - I I I I I 15-25 cm - ß ' . . -. . ß . . .\"' ..... . -'-... ß .'' . '\" . . ß ..... 237 241 245 249 253 Day of year Figure 10. Observed (dotted line) and simulated diurnal variation of soil temperature at old jack pine site. Bold solid line indicates assumed presence of mineral soil only; thin solid line indicates assumed presence of mineral soil with surface organic layer. 14,352 EL MAAYAR ET AL.: VALIDATION OF IBIS 800 600 400 200 o -200 Rn IBIS IBIS+osl a ß b -200 0 200 400 600 800-200 0 200 400 600 800 6OO , , 500 ?   400  : 300 x:  200 '  100 E o r.  -tOO -200   H IBIS IBIS+osl , d - _ -200-tOO 0 tOO 200 300 400 500 600-200-tOO 0 tOO 200 300 400 500 600 400 300 200 100 o -tOO t0 5 0 -5 -15 -20 - LE IB - IBIS+o. sl o ß - .  ? : :-.    .i  -   _ ' ' ' e -. ß .:: , . 5\" ':  :' - t 00 0 t 00 200 300 400 - t 00 0 t 00 200 300 400 Observed (W m -2) Observed (W m -2) NEE IBIS IBIS+osl g -2o - 5 -lo -5 o s lo 15 -2o -15 -lo -5 o 5  o  5 Observed (gmol-CO 2 m -2 s -1) Observed (gmol-CO 2 m -2 s -1) Figure 11. Simulated hourly above-canopy fluxes plotted against data observed at the old jack pine site during the period April 1 to October 9, 1996. (a) Net radiation assuming presence of mineral soil only, (b) mineral soil with surface organic layer. (c) Sensible heat flux assuming presence of mineral soil only, (d) mineral soil with surface organic layer. (e) Latent heat flux assuming presence of mineral soil only, (f) mineral soil with surface organic layer. (g) Net ecosystem exchange (NEE) assuming presence of mineral soil only, (h) mineral soil with surface organic layer. Carbon flux (NEE) is positive toward the atmosphere. from different boreal forest types obtained in the BOREAS experiment. The results showed both successes and deficiencies in IBIS' ability to simulate exchanges of mass and energy over boreal ecosystems. Although evapotranspiration was generally simu- lated reasonably well, sensible heat fluxes were systematically underestimated. The latter problem was more evident at a mature deciduous forest site (SOA) than at coniferous sites EL MAAYAR ET AL.: VALIDATION OF IBIS 14,353 20 10 -10 20 10 0 -113 20 10 5 0 -5 10 -5 I t 90 110 130 150 25-50 cm 50-100 cm .. I I I I I 170 Day of year 190 210 230 250 270 Figure 12. Observed (dotted line) and simulated daily soil temperature at old black spruce site. Thick solid line indicates assumed presence of mineral soil only; thin solid line indicates assumed presence of mineral soil with surface organic layer. (SOJP and NOBS). A sensitivity test and comparison with measured canopy heat storage data showed that this problem could be related to the physical parameterizations used to represent heat transfer between vegetation and atmosphere. Evidently, further work is required to improve the representa- tion of canopy heat storage in the model. Net ecosystem exchange of carbon (NEE) was generally simulated acceptably, although for the SOA site, summer and winter estimates showed appreciable bias compared to the means of all data (see Table 2). Furthermore, midday assimi- lation was generally overestimated, which appears to be due to underestimation of daytime respiration rates. The origin of this problem is not easy to determine: it could result from under- estimation of soil respiration temperature coefficients (we do not have measured soil respiration data), or it could be due to undereslimating soil carbon content (see above, section 5.1.). Future analyses based on field measurements are required. Careful validation of the soil biogeochemistry component of IBIS against extensive field measurements of soil respiration should to help to resolve this problem. Simulated ecosystem respiration was also evidently overes- timated during the winter period at SOA. This, combined with a general tendency to overestimate nighttime respiration, may suggest that the temperature responses for respiration (of soil and/or vegetation) are too shallow. Furthermore, for a better evaluation of NEE simulated by such DGVMs, more complete understanding is needed of the problems in using eddy corre- lation over tall canopies at nighttime when wind speeds are low, available energy is small and atmospheric stability is high [e.g., Lee, 1998; Baldocchi et al., 1998]. Hence it is to be ex- pected that the model can be further improved as technical measurement problems are resolved or alternative techniques are developed. Both observed and simulated mean Bowen ratios for conif- erous sites (SOJP and NOBS) were greater than 1.0, whereas those for the deciduous sites were typically much lower. This demonstrates that IBIS is able to reproduce correctly one of the fundamental differences between deciduous and conifer- dominated boreal ecosystems. The importance of predicting these differences in the Bowen ratio successfully is related to the influence of H and LE on mesoscale and local weather conditions (see the review of Pielke et al. [1998] and Hogg et al. [2000]). This implies that IBIS simulations of changes in veg- etation, e.g., due to global warming effects on species compe- tition and physiology, will lead to changes in the surface fluxes used as lower boundary conditions when IBIS is coupled to a GCM. The results of this study also showed the importance of including an organic layer in simulating surface energy carbon fluxes for boreal forest stands. The presence of surface organic material affects soil moisture and temperature, as well as soil heat flux, soil thawing, surface energy partitioning, and sur- 14,354 EL MAAYAR ET AL.: VALIDATION OF IBIS face-atmosphere carbon exchange. For instance, inclusion of the OSL in the model led to appreciable improvements in simulated soil heat flux and surface temperature, providing an additional explanation for why existing land surface models tend to overestimate soil \"skin\" temperature and downward soil heat flux. Betts et al. [1993] and Chen et al. [1997] related this problem to the numerical algorithms adopted to solve the surface energy balance (see also Beljaars [1991] for numerical details). Results for soil temperature at the NOBS site also showed that the inclusion of a surface organic layer delays the start of thawing, which in turn affects soil moisture availability, although it is clear that with increasing depth, the simulation of this delay is much less satisfactory (see Figure 12d). This effect is of considerable interest because several studies have dem- onstrated the importance of correct estimation of soil moisture content on the Bowen ratio, which in turn affects the develop- ment of the atmospheric boundary layer, and hence both local and regional atmospheric conditions (an extensive review can be found in the work of Betts et al. [1996]). Moreover, Goulden et al. [1998] showed the importance of soil depth and thaw on boreal forest carbon balance. It will be particularly important in spatial modeling therefore that the physical characteristics of both mineral and organic soil layers be properly parameter- ized. In order to achieve this difficult goal a starting point could be to test land surface parameterizations at a range of sites, using measured data for the vertical distributions of soil texture, soil thermal and hydraulic properties, soil carbon con- tent, and root biomass. Unfortunately, extensive data sets con- taining reliable values for these variables are not generally available. Future field campaigns should attempt to report such information, as suggested also by Delire and Foley [1999]. For instance, some of the disagreement between observed and simulated soil temperature and moisture, and hence energy and carbon fluxes, obviously originates from the use of a con- stant soil texture profile in our simulations. Concerning surface organic material, Enrique et al. [1999] attempted to quantify the effect of plant-residue mulch on energy exchange between a grassland ecosystem and the atmosphere. A comparable, physically based, approach could be developed for forest can- opies, but for organic material in varying states of decomposi- tion. The importance of these effects of the organic surface layer on simulated exchanges of water and carbon is, of course, dependent upon its thickness. This study shows that consider- ation of the OSL in the model has only a minor effect on simulated water and carbon fluxes, for both deciduous and coniferous sites where the organic material thickness does not exceed a few centimetres. For the northern black spruce site, however, where the organic layer is 50 cm thick, the simulation of both latent heat flux and NEE were substantially improved when this was taken into consideration in the model. This study confirms and builds upon similar work by Delire and Foley [1999] who applied IBIS to other vegetation types including grassland and tropical forest ecosystems. Such stud- ies help to confirm the validity of the process components of IBIS and hence its value as a global ecosystem simulator. Although other aspects of the model still require validation, e.g., competition and phenology, validations such as ours have two major benefits. First, they increase confidence that the use of dynamic vegetation simulators will improve the representa- tion of land surface effects when coupled to GCMs, and hence allow climate modelers to improve predictions of how vegeta- tion feedbacks may affect climate as the climate changes. Sec- ond, they provide a very good basis for estimating the probable errors in simulations of canopy exchange processes at regional and global scales. Acknowledgments. We thank ENergy from the FORest (EN- FOR), funded by the Canadian Federal Panel on Energy Research and Development (PERD), who provided the financial support of this study. Brian Amiro, Robert Grant, Ted Hogg, and three anonymous reviewers provided careful reviews of an earlier version of this manu- script. AMS mesonet data were provided by the Saskatchewan Re- search Council. We wish to thank M. Goulden and D. Baldocchi for making, respectively, NOBS and SOJP data available to the BOREAS research community. References Baldocchi, D. D., C. A. Vogel, and B. Hall, Seasonal variation of carbon dioxide exchange rates above and below a boreal jack pine forest, Agr/c. For. Meterol., 83, 147-170, 1997a. Baldocchi, D. D., C. A. Vogel, and B. Hall, Seasonal variation of energy and water vapor exchange rates above and below a boreal jack pine forest, J. Geophys. Res., 102(D24), 28,939-28,952, 1997b. Baldocchi, D., K. Wilson, and K. T. Paw U, On measuring net ecosys- tem carbon exchange in complex terrain over tall vegetation, paper presented at 23 rd Conference on Agricultural and Forest Meteorol- ogy, Nov. 2-6, Am. Meteorol. Soc., Albuquerque, N.M., 1998. Ball, J. T., I. E. Woodrow, and J. A. Berry, A model predicting sto- matal conductance and its contribution to the control of photosyn- thesis under different environmental conditions, in Progress in Pho- tosynthesis Research, vol. 4, edited by J. Biggins, pp. 221-224, Martinus-Nijhoff, Zoetermeer, Netherlands, 1986. Beljaars, A. C. M., Numerical schemes for parameterizations, in Nu- merical Methods in Atmospheric Models, vol. 11, pp. 1-42, Eur. Cent. for Medium Range Weather Forecasts, Reading, England, Sept. 1991. Bellisario, L. M., L. D. Boudreau, D. L. Verseghy, W. R. Rouse and P. D. Blanken, Comparing the performance of the Canadian Land Surface-Scheme (CLASS) for two subarctic terrain types, Atmos. Ocean, 38(1), 181-204, 2000. Bessemoulin, P., and D. Puech, BOREAS TF-06 SSA-YA Surface energy flux and meteorological data, http://www-eodis.ornl.gov/, Distrib. Active Archive Cent., Oak Ridge Laboratory, Oak Ridge, Tenn., 1998. Betts, A. K., J. H. Ball, and A. C. Beljaars, Comparison between the land surface response of the European Centre Model and the FIFE- 1987 data, Q.J.R. Meteorol. Soc., 119, 975-1001, 1993. Betts, A. K., J. H. Ball, A. C. Beljaars, M. J. Miller, and P. Viterbo, The land-surface-atmosphere interaction: A review based on observa- tional and global modeling perspectives, J. Geophys. Res., 101(D3), 7209-7225, 1996. Black, T. A., and Z. Nesic, Boreal forest atmosphere interactions: Exchanges of energy, water vapor and traces gases, Distrib. Active Archive Cent., Oak Ridge Natl. Lab., Oak Ridge, Tenn., 1998. (Available at http://www_eodis.ornl.gov) Black, T. A., G. Den Hartog, H. H. Neumann, P. D. Blanken, P. C. Yang, C. Russell, Z. Nesic, X. Lee, S. G. Chen, R. Staebler, and M.D. Novak, Annual cycles of water vapour and carbon dioxide fluxes in and above a boreal aspen forest, Global Change Biol., 2, 159-168, 1996. Bonan, G. B., D. Pollard, and S. L. Thompson, Effects of boreal forest vegetation on global climate, Nature, 359, 716-718, 1992. Brutsaert, W., Evaporation into the Atmosphere, 299 pp., D. Reidel, Norwell, Mass., 1982. Calvet, J. C., J. Noilhan, J.-L. Roujean, P. Bessemoulin, M. Ca- belguenne, A. Olioso, and J.-P. Wigneron, An interactive vegetation SVAT model tested against data from six contrasting sites, Agric. For. Meteorol., 92, 73-95, 1998. Campbell, G. S., and J. M. Norman, An Introduction to Environmental Biophysics, 286 pp., Springer-Verlag, New York, 1998. Chen, T. H., et al., Cabauw Experimental results from the Project for Intercomparison of Land-surface Parameterization Schemes, J. Clim., 10, 1194-1215, 1997. Chen, W. J., et al., Effects of climatic variability on the annual carbon EL MAAYAR ET AL.: VALIDATION OF IBIS 14,355 sequestration by a boreal aspen forest, Global Change Biol., 5, 41-53, 1999. Ciais, P., P. Tans, M. Trolier, J. White, and R. Francey, A large Northern Hemisphere terrestrial CO2 sink indicated by  3C/ 2C ratio of atmospheric CO2, Science, 269, 1098-1102, 1995. Clayton, J. S., W. A. Ehrlich, D. B. Cann, J. H. Day, and I. B. Marshall, Soils of Canada, vol. 2, Inventory, 239 pp., Res. Branch, Can. Dep. of Agric., Ottawa, Ontario, 1977. Collatz, G. J., J. T. Ball, C. Grivet and J. A. Berry, Physiological and environmental regulation of stomatal conductance, photosynthesis and transpiration: A model that includes a laminar boundary layer, Agric. For. Meteorol., 53, 107-136, 1991. Collatz, G. J., M. Ribas-Carbo, and J. A. Berry, Coupled photosyn- thesis-stomatal conductance model for leaves of C4 plants, Aust. J. Plant Physiol., 19, 519-538, 1992. Cuenca R. H., D. E. Strangel, and S. F. Kelly, Soil water balance in a boreal forest, J. Geophys. Res., 102(D24), 29,355-29,367, 1997. Delire, C., and J. A. Foley, Evaluating the performance of a land surface/ecosystem model with biophysical measurements from con- trasting environments, J. Geophys. Res., 104(D4), 16,895-16,909, 1999. Dickinson, R. E., A. Henderson-Sellers, P. J. Kennedy, M. F. Wilson, Biosphere-Atmosphere Transfer Scheme (BATS) for the NCAR CCM, Tech. Note NCAR/TN-275-STR, Natl. Cent. for Atmos. Res., 69 pp., Boulder, Colo., 1986. Enrique, G.-S., I. Braud, J.-L. Thony, M. Vauclin, P. Bessemoulin, and J.-C. Calvet, Modelling heat and water exchanges of fallow land covered with plant-residue mulch. Agric. For. Meteorol., 97, 151-169, 1999. Farquhar, G. D., S. von Caemmerer, and J. A. Berry, A biochemical model of photosynthetic CO2 assimilation in leaves of C3 species, Planta, 149, 78-90, 1980. Foley, J. A., J. E. Kutzbach, M. T. Coe, and S. Levis, Feedbacks between climate and boreal forests during the holocene epoch, Na- ture, 371, 52-54, 1994. Foley, J. A., I. C. Prentice, N. Ramankutty, S. Levis, D. Pollard, S. Sitch, and A. Haxeltine, An integrated biosphere model of land surface processes, terrestrial carbon balance, and vegetation dynam- ics, Global Biogeochem. Cycles,  0(4), 603-623, 1996. Gates, D. M., Plant-Atmosphere Relationships, 92 pp., Chapman and Hall, New York, 1993. Goulden, M. L., B.C. Daube, S. M. Fan, D. J. Sutton, A. Bazzaz, J. W. Munger, and S.C. Wofsy, Physiological responses of a black spruce forest to weather, J. Geophy. Res., 102(D24), 28,987-28,996, 1997. Goulden, M. L., et al., Sensitivity of boreal forest carbon balance to soil thaw, Science, 279, 214-217, 1998. Gower, S. T., J. G. Vogel, J. M. Norman, C. J. Kucharik, S. J. Steele, and T. K. Stow, Carbon distribution and aboveground net primary production in aspen, jack pine, and black spruce stands in Saskatche- wan and Manitoba, Canada, J. Geophy. Res., 102(D24), 29,029- 29,041, 1997. Guyot, G., Climatologie de l'Environnement, 505 pp., Masson, Paris, 1997. Henderson-Sellers, A., and V. B. Brown, Project of the Intercompari- son of Land-surface Parameterization Schemes (PILPS): First sci- ence plan, IGPO PuN. Set., vol. 5, 53 pp., 1992. Henderson-Sellers, A., K. McGuffie, and A. J. Pitman, The project for Intercomparison of Land-surface Parameterization Schemes (PILPS): 1992 to 1995, Clim. Dyn., 12, 849-859, 1996. Hogg, E. H., D. T. Price, and T. A. Black, Postulated feedbacks of deciduous forest phenology on seasonal patters in the western Ca- nadian interior, J. Clim.,  3(24), 4229-4243, 2000. Jackson, R. B., J. Canadell, J. R. Ehleringer, H. A. Mooney, O. E. Sala, and E. D. Schulze, A global analysis of root distribution for terres- trial biomes, Oecologia, 108, 389-411, 1996. Kimball, J. S., P. E. Thornton, M. A. White, and S. W. Running, Simulating forest productivity and surface-atmosphere carbon ex- change in the BOREAS study region, Tree Physiol., 17, 589-599, 1997. Kucharik, C. J., J. A. Foley, C. Delire, V. A. Fisher, M. T. Coe, J. Lenters, C. Young-Molling, N. Ramankutty, J. M. Norman, and S. T. Gower, Testing the performance of a dynamic global ecosystem model: Water balance, carbon balance and vegetation structure, Global Biogeochem. Cycles,  4(3), 795-825, 2000. Larson, J. A., The Boreal Ecosystem, 500 pp., Academic, San Diego, Calif., 1980. Lee, X., On micrometeorological observations of surface-air exchange over tall vegetation, Agric. For. Meteorol., 91, 39-49, 1998. Loyd, J., and J. A. Taylor, On the temperature dependence of soil respiration, Functional Ecol., 8, 315-323, 1994. Manabe, S., and K. Bryan, Climate calculations with a combined ocean-atmosphere model, J. Atmos. Sci., 26, 786-789, 1969. Manabe, S., and R. T. Wetheraid, Large-scale changes of soil wetness induced by an increase in atmospheric carbon dioxide, J. Atmos. Sci., 44, 1211-1235, 1987. Nijssen, B., I. Haddeland, and D. P. Lettenmaier, Point evaluation of a surface hydrology model for BOREAS, J. Geophys. Res., 102(D24), 29,367-29,378, 1997. Pielke, R. A., and P. L. Vidale, The boreal forest and the polar front, J. Geophys. Res., 100(D12), 25,755-25,758, 1995. Pielke, R. A., T. J. Lee, J. H. Copeland, J. L. Eastman, C. L. Ziegler, and C. A. Finley, Use of USGS-provided data to improve weather and climate simulations, Ecol. Appl., 7, 1053-1069, 1997. Pielke, R. A., R. Avissar, M. Raupach, A. J. Dolman, X. Zeng, and A. S. Denning, Interactions between the atmosphere and terrestrial ecosystems: Influence on weather and climate, Global Change Biol., 4, 461-475, 1998. Pollard, D., and S. L. Thompson, Use of a land-surface-transfer scheme (LSX) in a global climate model: The response to doubling stomatal resistance, Global Planet. Change, 10, 129-161, 1995. Satterlund, D. R., An improved equation for estimating long-wave radiation from the atmosphere,  5(6), 1649-1650, 1979. Schneider, S. H., and R. E. Dickinson, Climate modeling, Rev. Geo- phys., 12, 447-493, 1974. Sellers, P. J., Y. Mintz, Y. C. Sud, and A. Dalcher, A Simple Biospher model (SiB) for use within general circulation models, J. Atmos. Sci., 43, 505-531, 1986. Sellers, P. J., D. A. Randall, G. J. Collatz, J. A. Berry, C. B. Field, D. A. Dazlich, C. Zhang, G. D. Collelo, and L. Bounoua, A revised land surface parameterization (SiB2) for atmospheric GCMs, part I, Model formulation, J. Clim., 9(4), 676-705, 1996. Sellers, P. J., et al., BOREAS in 1997: Experiment overview, scientific results, and future directions, J. Geophys. Res., 102(D24), 28,731- 28,769, 1997. Shao, Y., and A. Henderson Sellers, Modeling soil moisture: A project for Intercomparison of Land Surface Parameterization Schemes Phase 2(b), J. Geophys. Res., 101(D3), 7227-7250, 1996. Shewchuk, S. R., Surface mesonet for BOREAS, J. Geophys. Res., 102(D24), 29,077-29,082, 1997. Shukla, J., and Y. Mintz, Influence of land-surface evapotranspiration on the Earth's climate, Science, 215, 1498-1501, 1982. Steele, S. J., S. T. Gower, J. G. Vogel, and J. M. Norman, Root mass, net primary production and turnover in aspen, jack pine and black spruce forests in Saskatchewan and Manitoba, Canada, Tree Physiol., 17, 577-587, 1997. Tans, P. P., I. Y. Fung, and T. Takahachi, Observational constraints on the global atmospheric CO2 budget, Science, 247, 1431-1438, 1990. Verma, S. B., J. Kim, and R. J. Clement, Momentum, water vapor, and carbon dioxide exchange at a centrally located prairie site during FIFE, J. Geophys. Res., 97, 18,629-18,639, 1992. Verseghy, D. L., N. A. McFarlane, and M. Lazare, CLASS-A Cana- dian land surface scheme for GCMs, II, Vegetation model and coupled runs, Int. J. Climatol., 13, 347-370, 1993. P. Bessemoulin, Maltrio-France, Service Central d'Exploitation de la Mdtdorologie, 42 Avenue G. Coriolis, 31057 Toulouse Cddex, France. A. Black, Department of Agroecology, University of British Colum- bia, Vancouver, BC, Canada V6T 124. C. Delire and J. A. Foley, Center for Sustainability and the Global Environment, Institute for Environmental Studies, University of Wis- consin, 1225 West Dayton Street, Madison, WI 53706. M. E1Maayar and D. T. Price, Natural Resources Canada, Canadian Forest Service, 5320-122 Street, Edmonton, AB, Canada T6H 3S5. ( e lmaay ar @nrcan.gc. ca) (Received May 31, 2000; revised February 20, 2001; accepted February 27, 2001.) 


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