JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 116, D09108, doi:10.1029/2010JD015224, 2011 Diagnosing the equilibrium state of a coupled global biosphere‐ atmosphere model Shanshan Sun1 and Guiling Wang1 Received 22 October 2010; revised 11 February 2011; accepted 21 February 2011; published 12 May 2011. [1] This study combines a conceptual modeling approach and a physical process–based modeling approach to diagnose and understand the equilibrium state(s) of coupled biosphere‐atmosphere models using the NCAR CAM3‐CLM3‐DGVM model as an example, with a focus on the West Africa and South America regions. First, a conceptual model is parameterized according to results from offline simulations using CAM3‐CLM3 and CLM3‐DGVM. The resulting conceptual model is then used to predict the potential biosphere‐atmosphere equilibrium state(s) for the coupled CAM3‐ CLM3‐DGVM model. Finally, simulations using the coupled CAM3‐CLM3‐DGVM model itself are carried out to verify the results of the conceptual model. Only one equilibrium state is found in both the conceptual model and the physically based numerical model. The CLM3 model features excessively high soil evaporation and very low plant transpiration, which leads to high bare‐ground ET and low sensitivity of ET to vegetation cover changes in the land model. Despite the high sensitivity of precipitation to evapotranspiration changes in the atmospheric model, the land model deficiency leads to a high amount of precipitation in the absence of vegetation cover and a low sensitivity of precipitation to vegetation changes in CAM3‐CLM3, two conditions that are found to anchor a coupled biosphere‐atmosphere model to a single equilibrium state. This statement also holds for the up‐to‐date version of the models using CLM4. This study provides an example for the importance of land surface processes in determining the potential equilibrium states of fully coupled biosphere‐atmosphere models. Citation: Sun, S., and G. Wang (2011), Diagnosing the equilibrium state of a coupled global biosphere‐atmosphere model, J. Geophys. Res., 116, D09108, doi:10.1029/2010JD015224. 1. Introduction [2] Past numerical modeling studies have identified terrestrial biosphere‐atmosphere interaction as one mechanism that can lead to multiple equilibrium states in the climate system [e.g., Charney, 1975; Claussen, 1998; Wang and Eltahir, 2000a; Oyama and Nobre, 2003]. Under current climate conditions, these modeling studies have identified the Sahel and the Amazon border areas as potential regions possessing multiple equilibrium states attributable to biosphere‐ atmosphere interactions. In these regions, vegetation growth is limited by water availability; and vegetation cover changes can exert significant impact on land‐atmosphere interactions and modify local climate conditions. Specifically, by increasing surface albedo and Bowen ratio and decreasing surface roughness, desertification or deforestation could reduce local precipitation through their impact on surface water and heat fluxes, net radiation, and large‐scale circulation as well. The 1 Department of Civil and Environmental Engineering and Center for Environmental Sciences and Engineering, University of Connecticut, Storrs, Connecticut, USA. Copyright 2011 by the American Geophysical Union. 0148‐0227/11/2010JD015224 reduction in precipitation may cause further degradation of vegetation, leading to a positive feedback. This positive feedback between vegetation and precipitation might give rise to long‐lasting drought and push the land‐atmosphere system into a drier equilibrium state. [3] In the Sahel region and Amazon borders area, simulated precipitation is found to be very sensitive to prescribed changes in vegetation cover [e.g., Claussen, 1998; Oyama and Nobre, 2004], a climate characteristic of regions prone to multiequilibrium states [Wang, 2004; Liu et al., 2006]. Consistently, multiequilibrium states have been found to exist in these regions in various climate models, including models with asynchronous vegetation‐climate coupling [Claussen, 1997, 1998; Oyama and Nobre, 2003] and models with synchronous vegetation‐climate coupling [Wang and Eltahir, 2000a, 2000b; Zeng and Neelin, 2000; Zeng et al., 2002; Wei et al., 2006]. [4] In addition to physically based numerical climate models, conceptual models with as few as two variables (one representing the atmosphere and the other the biosphere) have also been developed and used to study the multiequilibrium behaviors resulting from biosphere‐ atmosphere interactions [Svirezhev and Bloh, 1996; Brovkin et al., 1998; Zeng et al., 1999; Da Silveira Lobo Sternberg, D09108 1 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM 2001; Wang, 2004]. Conceptual models’ advantages lie in their highly simplified representation of physical mechanisms, which makes results easier to interpret. In a conceptual model, depending on whether temperature, radiation, or water supply is the limiting factor for vegetation growth, the atmospheric state variable can be thermal, radiative, or hydrological. Although radiation is the limiting factor for the interior Amazon [e.g., Myneni et al., 2007], water is the main limiting factor for vegetation growth in the Sahel and Amazon boundary regions. Precipitation (P) is therefore used as the atmosphere state variable in conceptual models pertaining to these regions [Brovkin et al., 1998; Zeng et al., 1999; Da Silveira Lobo Sternberg, 2001; Wang, 2004]. Using vegetation density or leaf area index (LAI) as the biosphere variable in conceptual models, precipitation’s response to vegetation cover changes is represented by a P*(V) curve and vegetation’s response to precipitation is represented by a V*(P) curve. The climate equilibrium states can be identified by the intersections between these two curves. Regions with multiple equilibrium states are characterized by a high sensitivity of precipitation to local vegetation cover changes and a high sensitivity of vegetation to precipitation changes. [5] Combining the numerical modeling approach with the conceptual modeling approach, Wang [2004] parameterized the P*(V) and V*(P) curves of a conceptual model using outputs from a physically based stand‐alone zonally symmetrical atmospheric model and a dynamic vegetation model. The so defined conceptual model is then used to interpret and predict behaviors of the physically based, coupled zonally symmetrical model. Specifically, to derive the P*(V) curve, the atmospheric model was driven with different prescribed vegetation covers to simulate the response of precipitation to vegetation changes. To derive the V*(P) curve, the land model with dynamic vegetation was driven with different prescribed atmospheric forcings to simulate the response of vegetation to precipitation changes. The resulting conceptual model predicts two stable equilibrium states in the Sahel region, the wet one corresponding to the current condition and the arid one corresponding to a much drier and less productive condition. These two equilibrium states correspond extremely well with the two equilibrium states derived from the physically based coupled dynamic vegetation‐atmosphere model [Wang and Eltahir, 2000a; Wang, 2004]. [6] The Wang [2004] study demonstrated the usefulness of conceptual modeling as a tool to diagnose and understand behaviors of complex physically based models. However, the zonally symmetrical atmospheric model used by Wang [2004] was characterized by a very small magnitude of atmospheric interannual variability due to the lack of zonal wave disturbance and other simplifications. It remains questionable whether the same approach can be applicable to complex, commonly used global climate models, the behaviors of which are much more difficult to understand and to predict than those of a simplified model such as the one used by Wang [2004]. Using a coupled atmosphere‐ land‐dynamic vegetation model as an example, this study applies the Wang [2004] to a GCM and investigates how land surface processes may play a role in determining the number and state(s) of regional climate equilibrium, a topic D09108 that is critical for understanding and predicting runaway behaviors in the climate system. 2. Model Description [7] The models used in this study include the conceptual model of Wang [2004] and several physically based numerical models, including the National Center for Atmospheric Research (NCAR) Community Atmosphere Model version 3 (CAM3) coupled with the Community Land Model version 3 (CLM3) including the Dynamic Global Vegetation Model (DGVM) (CAM3‐CLM3‐DGVM) and its component models (i.e., CAM3‐CLM3 with static vegetation and CLM3‐DGVM). In addition, an updated model version CAM4‐CLM4 is also used to test the sensitivity of our results to recent implemented model parameterization changes. 2.1. The Conceptual Model [8] The two‐variable conceptual model includes four basic equations. The first two describe the dynamics of the biosphere (dV/dt = (V* − V)/t) and the stochastic nature of the atmosphere (P = P* + sR(t)). Here t is time, t is the characteristic time scale of vegetation variation. The two variables of the model are vegetation V as the biosphere state and precipitation P as the atmospheric state variable. V* stands for the vegetation state in equilibrium with precipitation P; P* stands for the precipitation amount in equilibrium with vegetation V. Precipitation P consists of two parts, P* as determined by vegetation and a stochastic component P′ = sR(t), in which s is the standard deviation of precipitation caused by atmospheric internal variability and the random time series R(t) follows standard normal distribution. [9] The other two equations of the conceptual model define V* and P* used in the first two equations. They represent the response of equilibrium vegetation to precipitation changes (the V* (P) curve) and the response of equilibrium precipitation to vegetation changes (the P* (V) curve), respectively. While analytical forms of the two equations can be used in theoretical studies on general biosphere‐atmosphere interactions, in this study the two equations will be derived based on output from the numerical models CAM3‐CLM3 and CLM3‐DGVM as the conceptual model is developed to describe the behaviors of the coupled model CAM3‐CLM3‐DGVM. While the first two equations are needed to describe climate variability, we will be primarily dealing with the P* (V) and V* (P) relationships in this study as the focus here is on diagnosing the equilibrium state(s) of the model. 2.2. CAM3‐CLM3‐DGVM and Its Component Models [10] The coupled biosphere‐atmosphere model CAM3‐ CLM3‐DGVM model is used to derive the equilibrium state (s) of the biosphere‐atmosphere system in different regions. The model simulates the dynamic land‐atmosphere system including vegetation dynamics under the present‐day solar irradiance and monthly varying climatological sea surface temperature (SSTs) [Hurrell et al., 2008]. At each time step, CAM3 simulates the atmospheric processes and provides atmospheric forcing to CLM3‐DGVM; driven with atmospheric forcing from CAM3, CLM3‐DGVM simulates the land surface biogeophysical, physiological, biogeochemical 2 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM processes and ecosystem dynamics, providing surface fluxes (sensible heat flux, latent heat flux (or evapotranspiration), and momentum flux) to CAM3 and updating the vegetation structure and distribution. For CAM3, the Eulerian spectral dynamical core is chosen with a T42 horizontal resolution and a total of 26 levels in the vertical direction. Details of the CAM3 model are provided by Collins et al. [2004], and the description for a more recent version CAM4 is provided by Neale et al. [2010]. [11] The component model CAM3‐CLM3 (or CAM4‐ CLM4) simulates the land‐atmosphere system while specifying a static vegetation condition. It is used in this study to derive the precipitation amount corresponding to different levels of prescribed vegetation conditions. Its land surface scheme CLM3 simulates the land surface biogeophysical and physiological processes. However, without DGVM, CAM3‐CLM3 does not include representation of biogeochemical processes and ecosystem dynamics. [12] The component model CLM3‐DGVM is used to derive the vegetation structure and distribution corresponding to a given atmospheric forcing. In addition to the land surface biogeophysical and physiological processes simulated in the land model, CLM3‐DGVM also simulates the biogeochemical processes and dynamics of natural vegetation, including growth, mortality, and competition [Levis et al., 2004]. The dynamic vegetation model is modified from the Lund‐Potsdam‐Jena (LPJ) DGVM [Sitch et al., 2003]. Biogeophysical and biogeochemical processes are simulated with a 20 min time step while plant phenology is evaluated daily. Vegetation structure and distribution are updated yearly based on the annual accumulation of carbon for each individual PFT. The following description focuses on land surface hydrological processes because they significantly influence the behavior of the coupled CAM3‐CLM3‐DGVM model pertaining to the focus of this study, as shown in section 3. [13] The land surface model CLM3 [Dai et al., 2003; Oleson et al., 2004] represents the land surface with ten soil layers, up to five snow layers and one vegetation layer. Land surface heterogeneity is characterized by allocating four types of patches in each grid cell (glacier, lake, wetland and vegetated). The vegetated patch may include some bare soil. Natural vegetation is represented as combinations of different plant function types, and ten plant functional types (PFTs) are considered: tropical broadleaf evergreen and deciduous trees, temperate needleleaf evergreen trees, temperate broadleaf evergreen and deciduous trees, boreal needleleaf evergreen and boreal deciduous trees, C4, C3 and C3 arctic grasses. In the presence of vegetation, the model evapotranspiration (ET) consists of three components, the soil evaporation, vegetation interception loss and transpiration, each of which is estimated using the bulk aerodynamic equation. Soil moisture in the top soil layer (1.75 cm) is used to scale the moisture availability for soil evaporation. Both precipitation characteristics and vegetation density (as quantified by leaf and stem area index) influence the amount of precipitation intercepted by vegetation, which limits the interception loss through its influence on the area of canopy surface that is wet. Transpiration is regulated by leaf stomatal conductance, which varies with solar radiation and rooting zone soil moisture through their impact on photosynthesis. D09108 [14] The improper partitioning of ET among its three components, including overestimation of soil evaporation and interception loss and underestimation of plant transpiration, is a known problem in CLM3 [e.g., Bonan and Levis, 2006; Lawrence et al., 2007; Wang and Wang, 2007; Oleson et al., 2008; Lawrence and Chase, 2009]. More recent versions of the model, CLM3.5 and CLM4, include modifications of various model parameterizations to address this problem [e.g., Oleson et al., 2007, 2010]. Among those considered are a soil resistance term or a litter resistance term to slow down soil evaporation, a more rapid drop of soil evaporation with top layer soil wetness, and a reduced fraction of precipitation that can be intercepted by vegetation canopy. These parameterization changes have led to a certain degree of model performance improvement in simulating the surface hydrological budget when tested in offline mode [e.g., Oleson et al., 2008; Lawrence et al., 2011]. However, it is not clear how they may influence the model behaviors pertaining to biosphere‐atmosphere equilibrium. 3. Methodology and Experimental Design 3.1. Main Experiments and Methodology [15] To derive the equilibrium state(s) of the biosphere‐ atmosphere system using the physically based numerical model, the coupled model CAM3‐CLM3‐DGVM is run for 200 years. At the end of each 200 year simulation, although carbon accumulation is not complete, a vegetative equilibrium is obtained. To evaluate the potential existence of multiple equilibrium states of the coupled model, two different initial vegetation conditions are experimented on, one with bare ground and the other with forest everywhere. In the forest initial condition run, vegetation is initialized to be tropical broadleaf evergreen trees in the tropics and temperate broadleaf cold deciduous trees in the extratropics. [16] Components of the physically based numerical model are used to parameterize the conceptual model of biosphere‐ atmosphere system. In order to parameterize the P*(V) curve in the conceptual model, CAM3‐CLM3 is used to simulate precipitation under different prescribed vegetation covers. In the P*(V)_global experiments, the land surface files are taken directly from the outputs of the 200 years CAM3‐CLM3‐DGVM run starting from bare ground, representing different stages of global vegetation distribution (which ranges from bare ground to grass dominance or to tree dominance where climate is suitable for trees to survive). To exclude the possible nonlocal impacts introduced by global vegetation cover changes, companion experiments for the P*(V) curve for two regions (P*(V)_Sahel and P*(V)_SE‐Amz) are also carried out, in which only vegetation cover in the region of interest ((15°N–20°N, 16°W–11°E) for the Sahel, and (18°S– 7°S, 47°W–36°W) for the SE Amazon) is modified while vegetation elsewhere is kept the same as the equilibrium state derived from the coupled CAM3‐CLM3‐DGVM simulation. Although these differences in the way vegetation is specified led to some subtle differences in local vegetation between the global and regional experiments, the difference is by all means very small. So the difference between the P*(V) curves based on the P*(V)_global experiments and those based on the regional experiments (P*(V)_Sahel or P*(V)_SE‐Amz) is primarily due to the impact of nonlocal vegetation cover changes on the regional climates. 3 of 14 D09108 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM Table 1. Summary of Experiments Model Components Experiments Category Fully coupled Experiment DGVM_offline Experiment Atmosphere Land Vegetation Experiment Length Number of Simulations CAM3 CLM3 DGVM 200 years One Prescribed atmospheric forcings; Different among simulations CAM3 CLM3 DGVM 200 years Six CLM3 20 years nine CAM3 CLM3 20 years six P*(V)_SE‐Amz Experiment CAM3 CLM3 20 years six ET_overwrite Experiment CAM3, with ET prescribed instead of simulated by CLM3 CAM4 CLM3 Static global vegetation covers, different among simulations Different static Sahel vegetation covers among simulations. Other regions share the same static vegetation covers Different static SE‐Amz vegetation covers among simulations. Other regions share the same static vegetation covers Same static vegetation cover globally among simulations 20 years six CLM4 Default vegetation cover globally 20 years one CAM4 CLM4 20 years one CAM4 CLM4 Default vegetation cover with LAI halved globally Bare ground globally 20 years one P*(V)_global Experiment P*(V)_Sahel Experiment CAM4‐CLM4_ctrl Experiment CAM4‐CLM4_05lai Experiment CAM4‐CLM4_bare Experiment [17] In order to parameterize the V*(P) curve in the conceptual model, CLM3‐DGVM model is used in DGVM_offline experiments to simulate the vegetation structure and distribution under different atmospheric forcings. The hourly atmospheric forcing including surface temperature, wind, specific humidity, pressure, precipitation and incident solar radiation is derived from the coupled CAM3‐CLM3 model outputs with data of each year treated as a different realization of the mean climate. CLM3‐ DGVM will cycle through 1 year’s atmospheric forcing data multiple times until a vegetative equilibrium state is reached. Each experiment is run for 200 years to ensure that vegetation distribution has come to equilibrium states in the Sahel and the Amazon southeastern boundary regions where C4 grass is the dominant vegetation species. Therefore the model will cycle through 1 year’s atmospheric forcing 200 times to simulate the corresponding vegetation distribution under this specific climate condition. [18] Based on the intersection(s) between the P*(V) and the V*(P) curves, the conceptual model predicts the equilibrium state(s) for the CAM3‐CLM3‐DGVM model. Comparison with the equilibrium state(s) derived from CAM3‐CLM3‐DGVM itself will then provide validation for the conceptual model and for the applicability of the conceptual model in interpreting behaviors of the physically based numerical model. 3.2. CAM4‐CLM4 Experiments [19] As shown later in section 4, the lack of precipitation sensitivity to vegetation changes in CAM3‐CLM3 is an important characteristic that dominates the behavior of the modeled biosphere‐atmosphere system. Extensive parameterization changes have been implemented in the latest version of the NCAR model, and some of them are likely to cause changes in the model precipitation sensitivity to vegetation cover changes. To test this, three sensitivity experiments using CAM4‐CLM4 are conducted, each specifying a different level of vegetation density. With the same prescribed SSTs forcing and land surface cover, the only difference among these three experiments is that LAI takes the default value in CAM4‐CLM4_ctrl, is reduced by half in CAM4‐CLM4_05lai, and is set to zero in CAM4‐ CLM4_bare. Such vegetation differences are applied at the global level. 3.3. ET_overwrite Experiments [20] An important pathway for vegetation to influence precipitation is through ET. The sensitivity of precipitation to vegetation changes therefore depends on both the sensitivity of ET to vegetation changes and the sensitivity of precipitation to ET changes, with the former being determined by the land surface model and the latter by the atmosphere model. ET_overwrite experiments using CAM3‐CLM3 are designed to test the precipitation sensitivity to ET changes, where the CLM3‐simulated ET (and therefore latent heat) flux is replaced by a specified flux when passed to CAM3. First, in a 1 year simulation using CAM3‐CLM3‐DGVM restarting from its equilibrium state, ET in every time step of the whole year was written to a data file; using CAM3‐ CLM3 with vegetation specified according to the equilibrium vegetation, six experiments were carried out in which the model read in the ET flux from the data file in every time step and specified the ET in CAM3 to be 20%, 60%, 80%, 100%, 120% and 160% of the read‐in values, respectively. That means at each time step, evapotranspiration provided to the atmosphere in CAM3 is prescribed, which replaces the actual evapotranspiration predicted by the land model CLM3. These six experiments are each 20 years long; in the same experiment, ET is specified the same from year to year with diurnal and seasonal cycles. The last ten model 4 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM D09108 Figure 1. Peak leaf area index distribution at the equilibrium state of the fully coupled CAM3‐CLM3‐ DGVM model, with the six study areas labeled using the open boxes. years’ outputs are used to analyze precipitation’s response to ET variations. [21] To summarize, Table 1 lists all experiments used in this study and how various parameters/parameterizations are treated. 4. Results [22] Experiments using the coupled CAM3‐CLM3‐ DGVM model initialized with drastically different initial vegetation conditions, one with bare ground and one with full forest cover, produced the same equilibrium state. The global patterns of precipitation and vegetation distribution at this equilibrium state are generally similar to the present‐day observations. Our results analysis here focuses on two broadly defined regions, West Africa and the Amazon region, which are further divided as shown in Figure 1. These two regions are chosen as their climates and circulation patterns are found to be sensitive to land surface condition changes in previous studies [e.g., Xue and Shukla, 1993; Zhang et al., 1996; Xue et al., 2006; Patricola and Cook, 2008; Alo and Wang, 2010], and two of the subareas, the Sahel area (15°N–20°N and 16°W–11°E) and the Amazon southeastern area (SE‐Amz, 7°S–18°S and 47°W– 36°W), were found to be prone to multiple equilibrium states attributable to vegetation‐climate interactions [Claussen, 1998; Wang and Eltahir, 2000a; Zeng and Neelin, 2000; Oyama and Nobre, 2003]. [23] Climate in West Africa is under the influence of the West African monsoon circulation. The rainy season in West Africa occurs during boreal summer, and its length decreases away from the Guinea coast northward. Annual precipitation and vegetation distribution in West Africa are characterized by strong gradient in the latitudinal direction, and the variation in the zonal direction is rather small. Except for the coastal region, vegetation in most areas of West Africa is limited by precipitation. On the contrary, in most areas of the Amazon, precipitation is abundant and does not show a strong spatial gradient, and vegetation is more limited by light availability. However, in the Amazon border areas, water is the limiting factor for vegetation growth. [24] Despite the overall agreement with observations in the general patterns of vegetation and precipitation distribution, discrepancy between the CAM3‐CLM3‐DGVM equilibrium and observations are found at the regional level. Compared with the climatic research unit (CRU) data [New et al., 2000], yearly precipitation is overestimated in West Africa and underestimated in South America including the Amazon. Correspondingly, in West Africa, the simulated C4 grass cover extends into the Sahara desert, while in the Amazon region tropical broadleaf deciduous tree and C4 grass cover is overestimated at the expense of evergreen tree coverage. [25] In two of the subareas (Sahel and SE‐Amz) at the equilibrium state of the coupled CAM3‐CLM3‐DGVM model, vegetation is dominated by grass, similar to present‐ day observations in the SE‐Amz region but represents an overestimation of grass coverage in the Sahel region. The other four subareas are densely forested at the equilibrium state of the fully coupled CAM3‐CLM3‐DGVM model, which is also similar to present‐day observations. For all six regions, spatial averages of peak leaf area index (PLAI) and yearly precipitation are used as the state variables for the biosphere and the atmosphere, respectively, in plotting the P*(V) and V*(P) curves for the conceptual model. The use of LAI as the state variable for the biosphere may present an issue when the dominant vegetation type differs within the precipitation range of the same V*(P) curve. For example, trees with a PLAI of 2 would require much more precipitation than grass with a PLAI of 2. However, this has not been a problem for the six subareas examined in this study. In addition, biomass was also tested as an alternative bio- 5 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM D09108 Figure 2. Conceptual models for the (a, c) Sahel region and (b, d) SE‐Amz region. Figures 2a and 2b are based on P*(V)_global experiments; Figures 2c and 2d are based on P*(V)_Sahel experiments and P*(V)_SE‐Amz experiments. Corresponding to each specific PLAI value, the five red circles represent annual precipitation in the last 5 years of the P*(V)_global experiment in Figures 2a and 2b, the P*(V)_Sahel experiment in Figure 2c, and the P*(V)_SE‐Amz experiment in Figure 2d, with the 5 year average shown by the black stars. Red line is the linear least square fit of red circles. Corresponding to each specific precipitation value, the blue triangle represents PLAI averaged over the last 10 years each DGVM_offline experiment. Blue line is the linear least square fit of blue triangles. The magenta solid circle in each panel represents the annual precipitation and PLAI averaged over the last 30 years of the coupled CAM3‐CLM3‐DGVM simulation. sphere variable and the results are consistent with results based on PLAI. [26] As shown in Figure 2, for both the Sahel region and the SE‐Amz region, the P*(V) and V*(P) curves have only one intersection, indicating that the conceptual models predict only one equilibrium state for the coupled CAM3‐ CLM3‐DGVM model. This is consistent with results of the CAM3‐CLM3‐DGVM experiments. As a comparison, the magenta circles in Figure 2 show the equilibrium state derived directly from CAM3‐CLM3‐DGVM itself. In both regions, the equilibrium state predicted by the conceptual model corresponds very well to the equilibrium derived from the coupled CAM3‐CLM3‐DGVM model. This agreement validates the methodology of parameterizing conceptual models based on GCM outputs. The constructed conceptual model can therefore provide useful indications of GCM behaviors. [27] As shown in Figure 2, in the P*(V)_global experiments in which vegetation covers vary globally, the multiyear average of precipitation (black asterisks) increases slightly and then fluctuates. Such precipitation changes however are not significant, and are much smaller in magnitude than the interannual variability of precipitation (Figure 2). The precipitation response to the LAI changes is therefore considered negligible in the Sahel and SE‐Amz regions. When vegetation is modified in the specific region only (Figure 2c for Sahel region and Figure 2d for SE‐Amz region as examples), precipitation shows a similar lack of response to vegetation cover changes. For both regions, P*(V) curves are almost the same between experiments with globally modified vegetation and those with regionally 6 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM modified vegetation. The number of intersection between P*(V) and V*(P) curves remains one, and the location of this intersection shifts only slightly. Note that while vegetation cover changes do influence nonlocal precipitation, such impact is in general small compared with the impact on local precipitation. [28] As indicated by Wang [2004], for a given V*(P) relationship, two factors influence the number of equilibrium solutions of the conceptual model: precipitation amount in the absence of vegetation and sensitivity of precipitation to vegetation changes. Specifically, low precipitation in the absence of vegetation (lower than what it takes to grow any vegetation) combined with low sensitivity of precipitation to land cover changes tends to favor one arid equilibrium state; low precipitation in the absence of vegetation combined with medium‐to‐high sensitivity of precipitation to land cover changes tends to favor two stable equilibrium states, an arid one and a wet one; high precipitation in the absence of vegetation (higher than what it takes for some grass to survive) favors one wet equilibrium state regardless of how sensitive the precipitation is to land cover changes. In Figure 2 for both regions, the precipitation amount in the absence of vegetation is very high, higher than what it takes for grass to survive, and the yearly precipitation shows very low sensitivity to vegetation changes. Compared with the P*(V) curves in previous studies that showed multiequilibrium states in the Sahel region [Brovkin et al., 1998; Wang, 2004], CAM3‐CLM3 seems to overestimate precipitation under bare‐ground condition and underestimate the sensitivity of precipitation to vegetation cover changes. As explained above, when precipitation in the absence of vegetation is high, only one stable equilibrium state can exist regardless of precipitation’s sensitivity to land surface changes. This same reason is also responsible for the lack of multiequilibrium states in the SE‐Amz region in the coupled model. [29] Note that the lack of interannual variability in the atmospheric forcing used for the V*(P) experiments may have led to some overestimation of vegetation coverage and potentially LAI in semiarid regions [Notaro, 2008]. While this may slightly influence the state of the equilibrium predicted by the conceptual model, it should have no impact on the number of equilibrium state(s) as the latter is so overwhelmingly determined by the location and shape of the P*(V) curve. [30] To understand the low sensitivity of precipitation to vegetation changes in CAM3‐CLM3, we examine how the most relevant hydrological variables and radiative variables (averaged for each region) vary with PLAI in the P*(V) experiments (Figure 3). In the Sahel region (first through third rows in Figure 3), precipitation increases as PLAI increases from zero to 0.8 and then fluctuates as PLAI continues to increase. Evapotranspiration (ET) responds similarly, leading to cooling as PLAI increases. Atmospheric moisture convergence decreases, probably as a result of cooler surface favoring divergence. ET is much larger in magnitude than the atmospheric moisture convergence, indicating that local evapotranspiration’s impact on precipitation is dominant. Surface runoff decreases slightly as PLAI increases from zero to 0.8 and does not vary much as PLAI further increases. Subsurface drainage responds similarly. Soil moisture in the rooting zone (e.g., in the top 7 D09108 soil layers totaling 80 cm for C4 grass) decreases as PLAI increases from zero to 0.8 as a result of plant uptake, and shows no detectable decrease as PLAI further increases. [31] For the three components of evapotranspiration, as PLAI increases from zero to 0.8, interception loss increases and vegetation transpiration increases while soil evaporation decreases. Similar to other variables, the impact of vegetation seems to saturate at PLAI equal to 0.8. The response of ET partition to vegetation changes is qualitatively consistent with our expectations. Quantitatively however, compared with data from Dirmeyer et al. [2006] (which is an observation‐driven multimodel product), the model’s water budget is problematic. Contribution to total evapotranspiration from vegetation transpiration is much smaller than those from soil evaporation and/or interception loss. Under well‐ vegetated conditions, soil evaporation is comparable with that of interception loss and both are about twice the magnitude of vegetation transpiration. This improper water budget can be caused by overestimation of interception loss, ground evaporation and underestimation of plant transpiration, all of which are well documented in previous studies [e.g., Bonan and Levis, 2006; Lawrence et al., 2007; Oleson et al., 2008]. The underestimation of vegetation transpiration and the low sensitivity of transpiration to PLAI changes especially when PLAI exceeds a certain threshold, combined with the overestimation of soil evaporation and interception loss, downplay the impact of vegetation on the hydrological process and reduces precipitation’s sensitivity to vegetation cover changes. [32] In the SE‐Amz region, compared with the Sahel region, the response of various hydrological and thermal variables to vegetation changes seems to saturate at a different level, at about PLAI equal to 2 (fourth through sixth rows of Figure 3). The responses of most variables to LAI changes in this region follow a pattern similar to those in the Sahel, with two exceptions. First, the sensitivity of precipitation and total ET to LAI changes is even lower, with negligible changes from bare soil to vegetated land. Second, opposite to the Sahel region, albedo in the SE‐Amz region increases with the increase of PLAI. Land surface albedo is a combination of vegetation albedo and soil albedo, and the latter depends on soil color and the top‐layer soil moisture. As explained by Mei and Wang [2010], in the Amazon region soil albedo is lower than grass albedo due to the dark soil color and high soil moisture content. In addition to the high evaporation from bare ground, this increase of albedo with LAI further downplays the sensitivity of precipitation to LAI changes in the SE‐Amz region. [33] In both regions, the model soil evaporation from bare ground is at a magnitude similar to the total ET over well vegetated land. This high soil evaporation leads to large amount of precipitation in the absence of vegetation, which favors one wet stable equilibrium state regardless of how sensitive precipitation might be to vegetation cover changes. Wallace et al. [1990] compared ET measured over bare ground and over fallow bush land in semiarid regions in West Africa, and found that ET over bare ground is much lower than over bush land except for during the hours immediately after a rain event. In the more recent versions of the Community Land model (CLM3.5 and CLM4), hydrological parameterization changes led to improved ET partitioning [e.g., Lawrence et al., 2007; Oleson et al., 2008; 7 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM D09108 Figure 3. Surface variables in the Sahel region (first, second, and third rows) and the SE‐Amz region (fourth, fifth, and sixth rows) in the P*(V)_global experiments (blue triangles) and P*(V)_Sahel experiments and P*(V)_SE‐Amz experiments (red circles). Stöckli et al., 2008; Lawrence et al., 2011]. However, even in CLM4 the ET contrast between bare ground and vegetated land is still low. As a result, the model precipitation in the absence of vegetation is still high in CAM4‐CLM4, and precipitation sensitivity to LAI changes is still low (Figure 6). [34] The companion P*(V)_Sahel and P*(V)_SE‐Amz experiments (results shown in red in Figure 3), in which only the vegetation in the Sahel region or the SE‐Amz region is modified through gradually increasing PLAI from zero while the rest of the globe shares the same vegetation distribution, are designed to exclude potential impacts on 8 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM D09108 Figure 4. Conceptual models for the (a) Guinean Coast region, (b) C – Amz region, (c) NW – Amz region, and (d) NE – Amz region, with the P*(V) curve based on the P*(V)_global experiments. Legend is the same as in Figure 2. precipitation from nonlocal vegetation changes. In the P*(V)_Sahel and P*(V)_SE‐Amz experiments, vegetation’s impacts on radiative processes and hydrological processes in the Sahel region and the SE‐Amz region are very similar to those in P*(V)_global experiments. [35] The same approach was applied to the four other areas in the Amazon region and West Africa region, including a densely vegetated inland area in central Amazon (C‐Amz, 4°S–9°S, 59°W–50°W), and other three tropical areas: NW‐Amz (4°S–9°N, 81°W–61°W), NE‐Amz (4°S–9°N, 64°W–47°W) and Guinean Coast (4°N–9°N, 16°W–11°E). Same as Sahel and SE‐Amz regions, C‐Amz, NE‐Amz, NW‐Amz and Guinean Coast regions have only one equilibrium state derived from the conceptual model, which corresponds well to equilibrium state in the coupled CAM3‐CLM3‐DGVM models (magenta dots in Figure 4). In these regions too, the regional climate is anchored to a single equilibrium state due to the excessive precipitation in the absence of vegetation and low sensitivity of precipitation to vegetation changes, characteristics that result from overestimation of bare soil evaporation and a partially related underestimation of sensitivity of evapotranspiration to vegetation changes (Figure 5). [36] To test whether precipitation’s sensitivity to vegetation cover changes has improved in the latest version of the models, results from CAM4‐CLM4 are shown in Figure 6 for all six regions. Compared with results in Figure 2, the definition of the Sahel region as shown in Figure 6 is extended southward by a few degrees in the CAM4‐CLM4 experiments to include more vegetated land. The P*(V) curves show that precipitation increases slightly as LAI increased from zero to default values in all six regions, with a precipitation sensitivity slightly higher than that shown in Figure 2 and Figure 4 for CAM3‐CLM3. However, the difference in the average annual precipitation among the three experiments is still very small compared with the large interannual variation of precipitation in the last 5 years of each experiment. In the offline CLM4, ET also shows low sensitivity to LAI changes. Therefore recently implemented model parameterization changes in CAM4 and CLM4 do not seem to completely address the lack of model precipitation sensitivity to vegetation changes. Compared with CLM3, CLM4 is generally wetter, and therefore the minimum precipitation required for plant establishment is lower in CLM4. V*(P) curves in the conceptual model will then shift slightly to the left. With the lack of sensitivity of 9 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM D09108 Figure 5. ET versus PLAI for the (a) Guinean Coast region, (b) C – Amz region, (c) NW – Amz region, and (d) NE – Amz region, based on averages over the last 5 years of the P*(V)_global experiments. precipitation to vegetation changes, the two curves in the conceptual model will therefore still have only one intersection point. Results related to biosphere‐atmosphere equilibrium as documented in this study are therefore not expected to qualitatively change if the experiments were carried out with the recently released version4 of the NCAR models. 5. Role of the Atmosphere Model [37] An important pathway for vegetation to influence precipitation is through ET. The sensitivity of precipitation to vegetation changes therefore depends on both the sensitivity of ET to vegetation changes and the sensitivity of precipitation to ET changes, with the former being determined by the land surface model and the latter by the atmosphere model. Therefore, it remains unclear whether the model deficiency related to surface water budget as documented in section 4 is the only cause for the lack of sensitivity of precipitation to vegetation changes, or whether correcting such model deficiency would make a difference in the number and/or state of the model equilibrium state(s). [38] The ET_overwrite experiments, in which ET is prescribed at 20%, 60%, 100%, 120% and 160% of the control values (see Table 1), are used to study precipitation’s sensitivity to ET changes. In Figure 7, the red line represents the P*(ET) curve and the magenta line marks the Y = X relation. In all six regions, precipitation is highly sensitive to ET changes as ET increases from 20% to 160% of the control ET, and this increase in most cases is more than the increase of local moisture supply. Depending on the hydrological regime, the response of moisture convergence (as an indicator of large‐scale circulation) can be substantial. With the exception of the Guinea Coast region, in five of the six regions examined, the P*(ET) curves are approximately parallel to the Y = X line when ET is below a certain threshold, indicating that the moisture convergence (therefore large‐scale circulation) is not sensitive to ET changes under very dry conditions. The precipitation changes therefore mainly result from changes of local moisture supply. As ET further increases beyond the threshold value, the slope of the P*(ET) curves becomes larger than 1, indicating that moisture convergence increases with ET. Therefore, under wetter conditions, in addition to the enhancement of local moisture supply, the increase of ET also leads to enhanced moisture supply from surrounding regions through changes in the large‐scale circulation. This threshold value is at about 100% of the control ET for the 10 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM D09108 Figure 6. P*(V) curves for the (a) Sahel region, (b) SE – Amz region, (c) Guinean Coast region, (d) C – Amz region, (e) NW – Amz region, and (f) NE – Amz region, based on CAM4‐CLM4_ctrl, CAM4‐CLM4_0.5lai and CAM4‐CLM4_bare experiments. Legend is similar to that in Figure 2. two dry regions (the Sahel and the SE‐Amz), and is at only 40–60% of the control ET for the three wetter regions (the C‐Amz, NW‐Amz and NE‐Amz regions). For the Guinean Coast region, the slope of the P*(ET) curve is less than 1 as ET increases from 20% to 60% and then becomes larger than 1 as ET further increases from 100% to 160%. So the moisture convergence here decreases first and then increases with the increase of ET. [39] The red brackets on the x axis of Figure 7 mark the range of ET in the P*(V)_global experiments (shown in Figure 3 and Figure 5) in which LAI varies widely, from zero to local vegetation growth capacities (1.6 for Sahel region; around 5.0 for NW‐Amz, NE‐Amz, SE‐Amz, Guinean Coast regions and around 7.0 for C‐Amz region). The low sensitivity of ET to vegetation changes combined with the high sensitivity of precipitation to ET changes indicates that the lack of precipitation response to vegetation changes and the high amount of precipitation in the absence of vegetation in the CAM model result primarily from the low sensitivity of ET to vegetation changes in the land model. Therefore, if in the land model the soil evaporation in the absence of vegetation is reduced and the sensitivity of ET to vegetation changes is increased, the model precipitation will become much more responsive to vegetation changes and the precipitation in the absence of vegetation will become much lower than it currently is. Such changes may lead to a change in the number of equilibrium states of the coupled biosphere‐ atmosphere system. 6. Conclusions and Discussion [ 40 ] The current study follows the approach of Wang [2004] to explore the potential for multiequilibrium states in a coupled biosphere‐atmosphere model using the NCAR CAM3‐CLM3‐DGVM model as an example. We parameterize the conceptual model of Wang [2004] using results from CAM3, CLM3 and its DGVM model, where the response of vegetation to precipitation changes is defined using results from CLM3‐DGVM driven with different atmospheric forcings (including precipitation) and the response of precipitation to vegetation changes is defined using results from CAM3‐CLM3 driven with prescribed vegetation covers. The resulting conceptual model predicts only one equilibrium state for each of six regions examined (including the Sahel region and the SE‐Amz region where two equilibrium states were found to exist in some models), 11 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM D09108 Figure 7. Precipitation.versus ET for the (a) Sahel region, (b) SE – Amz region, (c) Guinean Coast region, (d) C – Amz region, (e) NW – Amz region, and (f) NE – Amz region, based on average over the last 10 years of the ET_overwrite experiments. The blue asterisks mark results from the ET_overwrite 100% experiment, and the red brackets denote the ET ranges simulated in the P*(V)_global experiments for each region. which correspond well with the single equilibrium state for each region derived from the fully coupled CAM3‐CLM3‐ DGVM model. [41] Based on the conceptual model, the physical processes influencing the equilibrium state(s) of the coupled system are analyzed to understand why the CAM3‐CLM3‐ DGVM model simulates only one equilibrium state in the Sahel and SE‐Amz regions, and in several other regions as well. Different from some previous modeling studies [Brovkin et al., 1998; Zeng et al., 2002; Wang, 2004], precipitation in CAM3‐CLM3 is very high under bare‐ground condition and shows little sensitivity to vegetation cover changes, which work together to anchor the climate system to a single equilibrium state. The large magnitude of precipitation in the absence of vegetation and the low precipitation sensitivity result from the lack of sensitivity of total evapotranspiration to vegetation changes, whereas the latter is related to a deficiency of the land surface model in simulating the surface water budget including overestimation of the soil evaporation and the underestimation of the transpiration. This attribution is further confirmed by results from a set of ET‐overwriting experiments that show a high sensitivity of precipitation to prescribed evapotranspiration changes in CAM3 (which therefore eliminates the atmospheric model as a possible cause for the low precipitation sensitivity to vegetation changes). [42] In all regions examined, ET changes trigger a highly sensitive response of precipitation, which in some cases involves changes in large‐scale circulation as indicated by changes in the moisture convergence. Previous studies have pointed out that West Africa and South America precipitation is closely linked to interactions between local ET and large‐scale circulation. In most of West Africa, precipitation is associated with the summer monsoon circulation, and increase of local moisture supply (through vegetation and soil moisture changes) was found to favor a stronger monsoon circulation that penetrates further inland (thus increasing moisture convergence in the Sahel region) [e.g., Xue and Shukla, 1993; Zheng and Eltahir, 1998; Wang and Eltahir, 2000a]. Dynamically, interactions between increased ET and African easterly jet (AEJ) slow down AEJ and strengthen the low‐level westerly jet. Reduced moisture exports by AEJ and increased moisture imports by low‐level westerly jet 12 of 14 D09108 SUN AND WANG: BIOSPHERE‐ATMOSPHERE EQUILIBRIUM tend to increase precipitation in the Sahel [e.g., Patricola and Cook, 2008]. For the South America region, Xue et al. [2006] found that the partition between sensible and latent heat flux plays an important role in local monsoon simulation. When ET is lower, compensating increased sensible heat flux strengthens ventilation effect and lower moisture static energy (MSE) of land. Lower land MSE modifies moisture flux convergence and reduces precipitation. For the SE‐Amz region located in the Amazon boundary area, numerical modeling study of Oyama and Nobre [2004] focused on vegetation’s impacts on precipitation and shown that decreased roughness length by desertification strengthens low‐level westward flow. At the same time, decreased diabatic heating caused by ET reduction increases divergence. Their net effect is the reduction of moisture convergence and precipitation following desertification. [43] Various studies have tackled the issue of improper ET partitioning in CLM3.0 [Bonan and Levis, 2006; Lawrence et al., 2007; Oleson et al., 2007, 2008; Lawrence and Chase, 2009; Oleson et al., 2010], and the resulting modifications to hydrological parameterizations have been included in the latest version CLM4.0. Lawrence et al. [2007] found that suppressing the high soil evaporation and interception loss and boosting the low vegetation transpiration led to improved model performance in simulating precipitation in some areas especially in the southeastern United States. Lawrence and Chase [2009] shows that a more realistic ET partitioning in CLM improves precipitation simulation, reducing precipitation in bare regions as soil evaporation decreases and enhancing precipitation in vegetated boreal forests as vegetation transpiration increases. Our sensitivity experiments using both the offline CLM4 and CAM4‐CLM4 confirm previous findings on improved ET partitioning and surface water budget. However, the impact of such improvement on precipitation amount in the absence of vegetation and on precipitation sensitivity to vegetation changes seems small, and certainly is not enough to change the number of the biosphere‐atmosphere equilibrium in the coupled CAM‐CLM‐ DGVM model. [44] Conceptual modeling proves to be an effective tool to diagnose the ability of fully coupled land‐atmosphere models in simulating the equilibrium state(s) attributed to biosphere‐atmosphere interactions. For a fully coupled land‐ atmosphere model including vegetation dynamics, it takes hundreds of model years for the vegetation distribution to come to an equilibrium state globally, and multiple runs using the coupled model with different initial conditions are needed to determine whether the coupled model has one or multiple equilibrium states. Moreover, understanding and attributing these results are difficult due to the difficulty of separating the different feedback processes within a coupled model. Conceptual modeling provides a computationally efficient alternative that allows explicit and separate treatment of the land and atmosphere responses, thus providing better insight regarding the land and atmosphere processes that influence the number and state(s) of the biosphere‐ atmosphere equilibrium. In the current study, results from the conceptual model directly led to the identification of model characteristics (or deficiencies) that anchor the coupled numerical model to a single equilibrium state, which will guide our future effort to modify model sensitivity and D09108 behaviors in order to explore the potential for multiple equilibrium states in coupled biosphere‐atmosphere model. [45] Acknowledgments. 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