G Model AGMET-4203; No of Pages 11 Agricultural and Forest Meteorology xxx (2010) xxx–xxx Contents lists available at ScienceDirect Agricultural and Forest Meteorology journal homepage: www.elsevier.com/locate/agrformet Soil water stress and coupled photosynthesis–conductance models: Bridging the gap between conflicting reports on the relative roles of stomatal, mesophyll conductance and biochemical limitations to photosynthesis Trevor Keenan a,*, Santi Sabate a,b, Carlos Gracia a,b a b CREAF, Autonomous University of Barcelona (UAB), 08193 Barcelona, Spain Department of Ecology, University of Barcelona (UB), 08007 Barcelona, Spain A R T I C L E I N F O A B S T R A C T Article history: Received 28 September 2009 Received in revised form 4 December 2009 Accepted 9 January 2010 Various plant responses to water stress have been reported, but conflicting reports as to which limiting process is the most important and ecophysiologicaly relevant during water stressed periods make it difficult to confidently model terrestrial CO2 and water flux responses. It has become increasingly accepted that mesophyll conductance could play a role in regulating photosynthesis during periods of water stress. We adapt the Farquhar-BB-type canopy photosynthesis–conductance model coupling to incorporate mesophyll conductance, embed it in an ecophysiological forest model and use it to simulate the effects of seasonal soil water stress on canopy CO2 and water fluxes at a Mediterranean Quercus ilex forest. Tests of various hypotheses regarding the relative roles of stomatal conductance limitations (SCL), mesophyll conductance limitations (MCL) and biochemical limitations (BL) confirmed that during water stressed periods, applying only BL allows for the accurate simulation of CO2 and water fluxes. Neither SCL nor MCL alone could accurately reproduce the observed CO2 and water fluxes. However, a combination of both MCL and SCL was successful at reproducing water stress induced reductions in CO2 and water fluxes, suggesting that mesophyll conductance could bridge the gap between conflicting reports on the processes behind responses to water stress in the field. ß 2010 Elsevier B.V. All rights reserved. Keywords: Terrestrial modelling Photosynthesis model Drought stress Mesophyll conductance Mediterranean climate 1. Introduction Process-based models that incorporate the relevant ecosystem processes to successfully simulate the sensitivity of ecosystem functioning to drought stress at all relevant time scales are indispensable tools. Such models of natural vegetation can assess the influence of stresses on the photosynthetic capacity of plants (Centritto et al., 2003; Loreto et al., 2003; Loreto & Centritto, 2008) and predict the effects of climate change on photosynthesis (Rogers & Humphries, 2000), thus helping to assess the vulnerability of ecosystems. Moreover, they are the only available tool for scaling carbon assimilation up from the leaf to whole plant and/or ecosystem (Harley & Baldocchi, 1995; Niinemets & Anten, 2009). Previous modelling studies, however, have highlighted the lack of model skill, at site, regional and global scales, to successfully reproduce the effects of seasonal stress due to low soil water availability, in particular in Mediterranean ecosystems (Morales et al., 2005; Jung et al., 2007). * Corresponding author at: CREAF, Edfici C, Universidad Autonoma de Barcelona, 08193 Bellaterra, Spain. Tel.: +34 93 581 2915; fax: +34 93 581 4151. E-mail address: [email protected] (T. Keenan). Projections of climate change (IPCC, 2007) suggest that higher temperatures, and increased potential evapotranspiration, as well as changes in seasonal precipitation patterns, will aggravate the seasonal drought stress characteristic to Mediterranean ecosystems (Giorgi et al., 2004; Giorgi, 2006; Beniston et al., 2007). Soil water availability is already the main limiting factor to global plant photosynthesis (Nemani et al., 2003), in particular in arid or semiarid ecosystems within Mediterranean climate regions (Boyer, 1982). An increase in anomaly events such as the 2003 European drought could also increase the amount of stress experienced in many non-Mediterranean forest ecosystems in Europe. However, despite recent advances (e.g., Grassi & Magnani, 2005), the effect of soil water stress on photosynthesis, and the vulnerability of Mediterranean vegetation to climate change, will not be fully understood until we untangle the ecophysiological responses and the main limitations imposed by water stress on leaf photosynthesis (Loreto & Centritto, 2008). Many different approaches have been developed over the last two decades to simulate the CO2 and water fluxes of a forest ecosystem. These biogeochemical models assess mass and energy exchange between the canopy and the atmosphere by coupling the fluxes of CO2 and water vapour (Wang & Jarvis, 1990; Aber & Federer, 1992; Amthor, 1994; Baldocchi & Harley, 1995; De Pury & 0168-1923/$ – see front matter ß 2010 Elsevier B.V. All rights reserved. doi:10.1016/j.agrformet.2010.01.008 Please cite this article in press as: Keenan, T., et al., Soil water stress and coupled photosynthesis–conductance models: Bridging the gap between conflicting reports on the relative roles of stomatal, mesophyll conductance and biochemical limitations to photosynthesis. Agric. Forest Meteorol. (2010), doi:10.1016/j.agrformet.2010.01.008 G Model AGMET-4203; No of Pages 11 2 T. Keenan et al. / Agricultural and Forest Meteorology xxx (2010) xxx–xxx Farquhar, 1997). The leaf physiologically based photosynthesis model by Farquhar et al. (1980), linked with a stomatal conductance model (Jarvis, 1976; Ball et al., 1987; Collatz et al., 1991; Leuning et al., 1995) provides a theoretical framework for spatially scaling up fluxes from leaf to canopy level. This processbased model coupling has proven hugely popular, and accurately integrates the canopy functioning over time scales from seconds to years (e.g., Caldwell et al., 1986; Leuning et al., 1995; Williams et al., 1997; Wang & Leuning, 1998; Keenan et al., 2009). Although such models are capable of giving very accurate results, they are not efficient at dealing with all conditions, in particular with water stress (Kramer et al., 2002; Morales et al., 2005). It has recently been shown that part of the model deficiency is due to the assumption of the sole control of stomatal conductance limitations (SCL) over photosynthesis during water stressed periods (Keenan et al., 2009). The inclusion of empirical ‘nonstomatal’ limitations has been shown necessary to successfully model CO2 and water fluxes in water stressed environments (e.g., Colello et al., 1998; Reichstein et al., 2002, 2003; Rambal et al., 2003; Xu & Baldocchi, 2003), with both CO2 and water fluxes being accurately modelled during water stressed periods through the reduction of photosynthetic potential (BL) in line with reductions in soil water availability (Keenan et al., 2009). Such a BL represents the effect of drought on metabolic functioning (e.g., the activity of the Rubisco activase enzyme, denitrogenisation, etc.). These model results suggest that stomatal aperture is driven by photosynthetic demand, and that the stomata do not play an active role in the long term regulation of photosynthesis during water stressed periods. This is controversial, as stomata have been widely reported to play a strong role in regulating photosynthesis during water stress (see Lawlor & Cornic, 2002, for a review). The conclusions from most studies, in particular model studies, were reached without taking into account the possible effects of a finite and changeable mesophyll conductance (gm). CO2 which enters the inter-cellular spaces of the leaf through the stomata diffuses through the mesophyll to the site of carboxylation in the chloroplast. It is becoming increasingly accepted that gm is finite and variable (Warren, 2008a), and that the concentration of CO2 in the inter-cellular spaces (Ci) differs from the concentration of CO2 in the chloroplast (Cc) in a manner that is highly variable within species and affected by a range of environmental conditions (e.g., Flexas et al., 2007; Warren, 2008b). Limitations of photosynthesis due to changes in gm (MCL) could play a role in plant responses to water stress (Grassi & Magnani, 2005; Galmés et al., 2007; Warren, 2008b; Keenan et al., 2010). This strengthens the need to incorporate a term that considers gm in current photosynthesis models, such as that by Farquhar et al. (1980), thus calculating photosynthetic rates based on Cc instead of on Ci. It has been repeatedly suggested that gm should be included in models of photosynthesis. However, as yet, there is no simple and accurate way to predict gm without measuring it. This is because gm strongly varies among and within given species (Ethier and Livingston, 2004; Flexas et al., 2008; Niinemets et al., 2009a; Warren, 2008a). gm is affected by both leaf structure (e.g., mesophytic leaves with higher vs. sclerophytic leaves with lower gm (Evans et al., 2009; Flexas et al., 2008; Niinemets et al., 2009a; Terashima et al., 2006; Warren, 2008a) and many of the environmental variables that drive models of canopy photosynthesis (e.g., temperature, drought, etc. (Warren, 2008a)), and there is currently not enough physiological information for reliable parameterization of these dependencies. On the other hand, some of the environmental effects may be small or moderate relative to the overall effect of gm on canopy photosynthesis. For instance, the effect of temperature on gm has been reported to be relatively small (Niinemets et al., 2009a,b). Drought-dependent reductions have been shown to occur together with reductions in stomatal conductance (gs) (Centritto et al., 2003; Flexas et al., 2008; Loreto et al., 2003). In the current analysis, different hypothesis are tested, challenging current assumptions regarding the relative roles of SCL, MCL and BL to photosynthesis and conductance, and how to model them, during seasonal water stressed periods in the field. We modified the Farquhar et al. (1980) model to incorporate mesophyll conductance and thus calculated photosynthesis on a Cc basis. This was coupled to the widely used Leuning et al. (1995) version of the Ball-Berry conductance model (Ball et al., 1987), and embedded in the biogeochemical forest growth model GOTILWA+ (‘Growth Of Trees Is Limited by Water’) (Gracia et al., 1999; Keenan et al., 2008, 2009). We could therefore test the effect of the inclusion of a water stress responsive stomatal conductance, mesophyll conductance or photosynthetic potential on modelled CO2 and water fluxes. CO2 and water eddy-covariance flux data from the five year period from 2001 to 2005 at the Puechabon Mediterranean Quercus ilex forest site in France are used to test model performance during water stressed periods. 2. Materials and methods 2.1. Fluxnet site data Data and simulations refer to Puechabon State Forest study site, located 35 km NW of Montpellier (southern France) (38350 4500 E, 438440 2900 N, elevation 270 m). Vegetation is largely dominated by a dense over-storey of Quercus ilex trees (Allard et al., 2008). Due to its typical Mediterranean-type climate (with warm and wet winters, and hot and dry summers), the water content in summer falls regularly below the value at which water stress limitations to photosynthesis are expected (Rambal et al., 2003), leading to extended seasonal periods of drought stress. The timing and extent of drought conditions varies from year to year, depending on temperature and precipitation. The mean annual temperature is 13.5 8C with mean annual precipitation of 903 mm (Allard et al., 2008). Rooting depth is 4.5 m, with a maximum total soil water content of 210 mm (for the 4.5 m soil column) (Keenan et al., 2009; Grote et al., 2009; Rambal et al., 2003). Soil texture is silty clay loam (referring to the textural triangle, United States Department of Agriculture) homogeneous down to 0.5 m depth, with increasing rock content thereafter and a limestone rock base. For more details on the site see http://www.cefe.cnrs.fr/fe/puechabon/. Climate, and eddy-covariance CO2 and water (latent heat flux equivalent) flux Measurements from the period 2001 to 2005 are used, which had an average annual air temperature of 14.5 8C and average annual precipitation of 965 mm. The selected focus year 2002 was wetter (total precipitation 1166 mm) than the longterm average but was also warmer than average (average temperature for 2002 of 14.7 8C). The high soil water availability during spring, and the relatively high temperatures, led to high production in spring 2002. The corresponding high levels of production related transpiration, and a relatively dry summer which was uninterrupted by strong rainfall events led to a sharp and extended drought period during 2002. This contrast between high spring production and a prolonged uninterrupted summer drought makes 2002 at Puechabon a good example year to test different approaches to modelling soil water stress responses. The valid approaches for 2002 were then tested against the full time series. 2.2. Modified photosynthesis model with mesophyll conductance The photosynthesis model of Farquhar, von Caemmerer & Berry (1980) was modified to explicitly calculate mesophyll conductance Please cite this article in press as: Keenan, T., et al., Soil water stress and coupled photosynthesis–conductance models: Bridging the gap between conflicting reports on the relative roles of stomatal, mesophyll conductance and biochemical limitations to photosynthesis. Agric. Forest Meteorol. (2010), doi:10.1016/j.agrformet.2010.01.008 G Model AGMET-4203; No of Pages 11 T. Keenan et al. / Agricultural and Forest Meteorology xxx (2010) xxx–xxx and therefore accurately calculate the quantity of CO2 available for assimilation in the chloroplast, through a set of coupled equations. The Farquhar et al. (1980) model states that the rate of net photosynthesis (An) is the minimum of the carboxylation rate limited by the amount, activation state, and kinetic properties of Rubisco (Rubisco-limited Ac); and the carboxylation rate limited by the rate of RuBP regeneration (Electron transport limited Aj): An ¼ minfAc ; A j g (1) For Rubisco limited photosynthesis the net CO2 assimilation rate is limited by Ac: Ac ¼ Vcmax ðC c G pÞ C c þ ðK c ð1 þ ðOi =K o ÞÞÞ (2) where Cc is the concentration of CO2 in the chloroplast, Gp* is the photorespiratory CO2 compensation point in the absence of mitochondrial respiration, Vcmax is the maximum rate of Rubisco carboxylation, Oi is the O2 concentration, and Kc and Ko are the Michaelis–Menten constants describing carboxylation and oxygenation. For electron transport limited photosynthesis (Harley & Tenhunen, 1991): Aj ¼ ðJ=4Þ ðC c G pÞ C c þ ð2 G pÞ (3) where J is the rate of electron transport, dependent on irradiance, leaf temperature, and the capacity of electron transport (Jmax) (De Pury & Farquhar, 1997). These calculations of photosynthesis require the concentration of carbon in the chloroplast, which is a function of An, stomatal conductance (gs) and mesophyll conductance (gm). Traditional modelling approaches estimate stomatal conductance as a function of irradiance, the balance of the supply and demand of carbon, and vapour pressure deficit. Ball et al. (1987) proposed a semi-empirical stomatal model (BB model) in which stomatal conductance was expressed by the leaf photosynthetic rate, relative humidity over a leaf surface, and the ambient CO2 concentration, under conditions of ample water supply (Ball et al., 1987). This model was later developed by Leuning (1995) (BBL model) to include the effects of vapour pressure deficit and the CO2 compensation point (Leuning, 1995; Leuning et al., 1995): g s ¼ g s0 þ m An ðC a G Þð1 þ ðv pd=D0 ÞÞ (4) where gs (mol H2O m2 s1) is stomatal conductance to moisture, g s0 is the value of gs at the light compensation point (mol m2 s1), An is the rate of net photosynthesis (mmol m2 s1), C a is the atmospheric concentration of CO2 at the canopy surface (mmol mol1), G is the CO2 compensation point (mmol mol1), D0 (unitless) is an empirical coefficient that describes the sensitivity of conductance to vpd (vapour pressure deficit, kPa), and m is an empirical species-specific factor that specifies the baseline ratio between conductance and net photosynthesis (unitless). The concentration of carbon inside the chloroplast, Cc is then a function of the net photosynthesis (assimilation rate) An, stomatal conductance to CO2, gsc (=gs/1.6), and gm: An An Cc ¼ Ca (5) g sc gm where Ca (mmol mol1) is the atmospheric CO2 concentration and gm is the mesophyll diffusion conductance from the sub-stomatal cavities to the chloroplasts. This set of equations (Eqs. (1)–(5)) complete the mesophyll conductance based photosynthesis model, and are solved itera- 3 tively by closing the leaf energy balance through leaf temperature. Values for Kc, Ko, Oi and G* were taken from Bernacchi et al. (2001). Jmax and Vcmax were calculated following Farquhar et al. (1980) and De Pury and Farquhar (1997). The effect of the inclusion of gm in the Farquhar BB-type model coupling (for a non water stressed system) was conducted using three reference values for gm. This allowed for the reparameterization of the photosynthetic parameters Jmax and Vcmax (following Niinemets et al., 2009b). A gm of 0.2 mol m2 s1 corresponds to a relatively high rate of mesophyll conductance encountered in plants adapted to relatively moist growing environments. The values of gm applied of 0.1 and 0.05 mol m2 s1 correspond to moderately low diffusive conductance, and very low diffusive conductance (see Niinemets et al., 2009a; Galmés et al., 2007 for recent reviews of species gm values). gm = infinity refers to the original Farquhar et al. (1980) model, which assumes infinite mesophyll conductance. Many other factors have been suggested to affect gm, e.g., leaf age, environmental, ontogenic and genetic modification in leaf structure, salinity stress, water stress, radiation and VPD (see Flexas et al., 2008 for a review). There is as yet no consensus as to how such factors could be implemented when modelling with consideration of gm. There is good agreement in the literature of a temperature affect on gm at lower temperatures (<20 8C), but both positive and negative responses have been observed at higher temperatures (Bernacchi et al., 2002; Pons & Welschen, 2003; Warren & Dreyer, 2006; Yamori et al., 2006; Warren, 2008a). This is probably due to species specific temperature responses though available data is far from sufficient to construct temperature response of internal conductance (Warren, 2008a). As drought occurs typically during periods of high temperatures, we have omitted a temperature response of gm for this study. 2.3. The effect of soil water stress on coupled photosynthesis– conductance models Model studies have shown that the application of BL is sufficient to accurately model water stress affects on CO2 and water fluxes (Reichstein et al., 2002; Keenan et al., 2009), whilst it is commonly upheld that the stomata (SCL) (e.g., Tenhunen et al., 1990; Cornic, 2000), and the mesophyll (MCL) (e.g., Warren, 2008a; Keenan et al., 2010), play a strong role in regulating water stress responses (e.g., Grassi and Magnani, 2005, but see Loreto & Centritto, 2008). We test the following four hypotheses from the literature for the incorporation of the effect of drought stress on the (Farquhar—BB-type) coupled photosynthesis–conductance model: (1) Directly reducing photosynthesis in relation to reductions in soil water availability sufficiently constrains CO2 and water fluxes during water stressed periods (biochemical limitations, BL). This incorporates all reported non-conductance limitations. (2) Directly reducing stomatal conductance in relation to reductions in soil water availability is sufficient to explain variation in CO2 and water fluxes during drought stressed periods (stomatal conductance limitations, SCL). (3) Directly reducing mesophyll conductance in relation to reductions in soil water availability is sufficient to explain variation in CO2 and water fluxes during drought stressed periods (mesophyll conductance limitations, MCL). (4) A combination of conductance limitations (CL) can accurately simulate the observed flux data (CL = SCL + MCL). We tested the hypotheses by imposing the three limitations, either individually or combined, to: (a) photosynthetic potential Please cite this article in press as: Keenan, T., et al., Soil water stress and coupled photosynthesis–conductance models: Bridging the gap between conflicting reports on the relative roles of stomatal, mesophyll conductance and biochemical limitations to photosynthesis. Agric. Forest Meteorol. (2010), doi:10.1016/j.agrformet.2010.01.008 G Model AGMET-4203; No of Pages 11 4 T. Keenan et al. / Agricultural and Forest Meteorology xxx (2010) xxx–xxx (BL), (b) stomatal conductance (SCL), and (c) mesophyll conductance (MCL). Biochemical limitations were imposed by the direct reduction of photosynthetic potential through reducing both Vcmax and Jmax during water stressed periods, in line with the relative soil water content (as in Keenan et al., 2009): Vcmax ¼ Vcmax W facphoto ; Jmax ¼ J max W facphoto (6) where Vcmax and Jmax are the maximum rate of RuBP carboxylation, and the maximum rate of electron transport, respectively, and Wfacphoto is a soil moisture-dependent scalar with values between 0 and 1. This BL function directly reduces photosynthesis under drought stress, thus reducing the demand for CO2 and reducing conductance. Stomatal control of photosynthetic responses to drought stress is modelled through the application of a linear scalar of soil moisture, in a modified version of Eq. (4): mðAn Rd Þ g s ¼ W facstoma g s0 þ (7) ðC a G Þð1 þ ðv pd=D0 ÞÞ where Wfacstoma is a soil moisture-dependent scalar with values between 0 and 1. This SCL function results in a reduction in conductance with reductions in soil moisture, thus limiting the leaf internal CO2 available for photosynthesis. Mesophyll conductance limitations were modelled by applying a similar reduction function Wfacmeso to gm (g 0m ¼ W facmeso g m ). This MCL function thus results in a direct reduction in mesophyll conductance with reductions in soil moisture. The three limitation functions, Wfacphoto, Wfacstoma and Wfacmeso, have the following form: 8 1; if SðtÞ Smax < sðtÞ smin q W fac ¼ (8) ; if SðtÞ < Smax : smax smin where q is a measure of the non-linearity of the effects of soil water stress on physiological processes, smax the relative soil water content, for the 4.5 m soil column, at which reductions are first evident, and smin is the wilting point. For the sake of comparative simplicity, we have assumed that increases or decreases in limitation strength for a particular limitation (BL, SL, MCL) can be represented by changes in the q value. Thus smax and smin values are common to all limitation approaches (smax = 0.8, smin = 0.38 (168, 80 mm)). 2.4. The biosphere model platform The modified coupled Farquhar BB-type model was embedded in the ecophysiological model platform GOTILWA+ (Growth of Trees Is Limited by WAter) (Gracia et al., 1999; Keenan et al., 2008, 2009; www.creaf.uab.es/Gotilwa+). GOTILWA+ is a process based forest growth model that has been developed to simulate the processes underlying growth and to explore how these processes are influenced by climate, tree stand structure, management techniques, soil properties and climate change. The GOTILWA+ model provides the biogeochemical background, and canopy microclimatic conditions necessary for the simulation of CO2 and water fluxes from forests in different environments, for different tree species, and under changing environmental conditions. Canopy CO2 and water fluxes of a forest ecosystem are estimated using a two layer canopy photosynthetic model (Wang & Leuning, 1998), coupled with a hydrology model. Sun and shade leaves are considered in the photosynthesis submodel (Wang & Leuning, 1998; Dai et al., 2004), with intercepted radiation depending on the time of the day, leaf area angle and the canopy’s ellipsoidal distribution (Campbell, 1986). The Farquhar approach (Farquhar et al., 1980; Von Caemmerer and Farquhar, 1981) outlined in Eqs. (1)–(5) is used to calculate the hourly rate of photosynthesis, depending on the direct and diffuse radiation intercepted, the species specific photosynthetic capacities, and leaf temperature. Stomatal conductance is calculated using the Leuning et al. (1995) version of the Ball and Berry model (Ball et al., 1987) (Eqs. (4) and (7)). Soil water content is described as one layer. Precipitation inputs are reduced by leaf interception, which is evaporated (stem interception, or stemflow, is not evaporated, but directed to the soil). Drainage, runoff, evaporation and transpiration are each considered. Run-off is calculated as a percentage of precipitation, and depends on the soil hydraulic gradient and porosity of the soil upper layer. Drainage is calculated to be inversely proportional to fractional soil water content (as in Honeysett and Ratkowsky, 1989; Gracia et al., 1999). Surface evaporation only occurs when the canopy is not closed. Monospecific (even- or uneven-aged) stands are considered, with no under-story. Individual trees are aggregated into 50 DBH (Diameter at Breast Height) classes and calculations are performed for each class. Ecosystem CO2 and water fluxes are estimated using hourly meteorological forcing, whereas slower processes such as growth and other state variables are calculated daily. Site specific parameters were taken from available literature. Previous model applications at the Puechabon site are published as Keenan et al. (2007, 2008, 2009). 2.5. Simulation methodology used The inclusion of gm requires the recalibration of photosynthetic parameters (Niinemets et al., 2009b)—Simulations were run with each fixed gm value (0.2, 0.1, 0.05 mol m2 s1) for the year 2002 at Puechabon to assess the impact of the inclusion of gm in the Farquhar-Ball Berry model coupling. Soil water stress was not considered for these simulations (i.e. Soil water content = maximum soil water content at all times). Following this initial testing and parameter recalibration, gm was then set at 0.1 mol m2 s1, which corresponds to moderately low diffusion conductance as found in Quercus ilex (see Niinemets et al., 2009a for a review of species gm values). The corresponding Vcmax and Jmax values (after calibrating modelled carbon and water fluxes against the FLUXNET carbon and water flux data) were 51 and 70 mmol m2 s1, respectively. Independent simulations were then run with a dynamic soil water content to test the different water stress response hypotheses as outlined above. In simulations applying BL, gm was fixed at 0.1 mol m2 s1. For simulations applying MCL and/or SCL, Vcmax and Jmax were kept constant. In each case, the strength of the limitation was incrementally increased (see Eq. (8)) until the least square fit was satisfied for either the CO2 (net assimilation rate) or water (latent heat flux) fluxes, when compared against the FLUXNET data. The different hypotheses which proved valid for 2002 were then applied, without further calibration, in comparative simulations for the five year period from 2001 to 2005, and compared against FLUXNET CO2 and water flux data. 3. Results 3.1. The effect of the inclusion of mesophyll conductance on simulated CO2 and water fluxes Simulations using a gm of 0.2 or 0.1 mol m2 s1 compared well to results from the traditional gm = infinity approach, once the photosynthetic parameters (Vcmax, Jmax) were adjusted (Fig. 1). No Please cite this article in press as: Keenan, T., et al., Soil water stress and coupled photosynthesis–conductance models: Bridging the gap between conflicting reports on the relative roles of stomatal, mesophyll conductance and biochemical limitations to photosynthesis. Agric. Forest Meteorol. (2010), doi:10.1016/j.agrformet.2010.01.008 G Model AGMET-4203; No of Pages 11 T. Keenan et al. / Agricultural and Forest Meteorology xxx (2010) xxx–xxx significant differences were observable for daily assimilation rates or rates of transpiration between the gm = infinity and the gm = 0.2 (An t-stat = 1.02, p = 0.9; Ea t-stat = 0.9, p = 0.42) or gm = 0.1 (An tstat = 0.09, p = 0.92; Ea t-stat = 0.82, p = 0.41) simulations. For gm = 0.1 simulations, slight differences in assimilation and transpiration were observed only at high temperatures and high vpd when compared to the gm = infinity simulations. No change in water use efficiency was observed for gm = 0.1 simulations compared to gm = infinity simulations. Simulating with gm = 0.05 led to significant differences in daily assimilation rates (tstat = 3.2, p < 0.01), most notably at high temperatures and high vpd. Large significant differences (t-stat = 4.8, p < 0.001) were observed in daily transpiration rates between the gm = infinity, and gm = 0.05 simulations, due to increased water use efficiency (Fig. 1). These differences were larger at higher temperatures, radiation and high vpd values. 3.2. Hypotheses testing Testing of the first of the three hypotheses showed that the application of restrictions to photosynthetic potential (BL) allowed for the effective reproduction of both CO2 and water fluxes (Fig. 2) during the water stressed period in 2002 at Puechabon (An r2: 0.92, RMSE: 1.8; LHF r2: 0.66, RMSE: 1.8). Both the assimilation rate and the latent heat flux (equivalent to evapotranspiration) reduced in parallel when simulating with BL (Eq. (6)), thus conserving the water use efficiency (Fig. 3). The reduction of gs alone through the application of Wfacstoma (SCL: Eq. 7) reduced stomatal conductance (and thus the latent heat flux), but water use efficiency remained high due to increased assimilation rates (Fig. 3). This lead to a large overestimation of total assimilated carbon during the water 5 stressed period of 2002 (An r2: 0.7, RMSE: 8.9; LHF r2: 0.7, RMSE: 5.0). Implying mesophyll conductance limitations (MCL) through reducing gm during water stressed periods proved more effective at modelling the water stress induced drop in assimilation rates than did SCL, but less effective at simulating water fluxes (An r2: 0.75, RMSE: 4.5; LHF r2: 0.53, RMSE: 5.9) (Fig. 2). The application of MCL was most ineffective at reproducing fluxes at mild water stress (between RSW of 0.5 and 0.7), where water fluxes were accurately simulated but slight overestimations in water use efficiency (Fig. 3) led to a much higher predicted assimilation rate than that observed (Fig. 2). Our last hypothesis was that a joint combination of diffusive conductance limitations (CL), with no limitation of photosynthetic potential (constant Vcmax, Jmax), could match observed CO2 and water fluxes during water stressed periods. Setting both conductance limitations to be of equal strength (SCL = MCL) allowed for a moderately accurate simulation of water (latent heat flux equivalent) fluxes, but CO2 fluxes were not as well reproduced (Fig. 4a) (An r2: 0.48, RMSE: 6.9; LHF r2: 0.72, RMSE: 5.4). This follows from the results presented in Figs. 2 and 3, as SCL reduces conductance but is not sufficient to reduce photosynthesis even with an additional MCL of equal strength. Further independent increases in stomatal restrictions (SCL > MCL) could not reduce assimilation (Fig. 4b), and gave increased water use efficiency (see Fig. 3). An even further increase in SCL, leads to underestimated latent heat fluxes, and overestimated assimilation rates (data not shown). Applying stronger MCL than SCL allowed for an accurate simulation of both CO2 and water fluxes (Fig. 4c) (An r2: 0.82, RMSE: 3.0; LHF r2: 0.73, RMSE: 1.7). CO2 fluxes were not as accurately simulated as through the application of BL (Hypothesis Fig. 1. Modelled non water stressed responses of daily canopy net assimilation (An), transpiration (Ea, mm day1), and water use efficiency (WUE, mmol mol1) to temperature (T, 8C), global radiation (MJ m2 day1), and vapour pressure deficit (VPD, kPa) for different values of mesophyll diffusion conductance (gm, mol m2 s1), at the Puechabon Forest in 2002. Simulations were run using the coupled Farquhar BB-type model coupling, embedded in the GOTILWA+ forest model (Keenan et al., 2008, 2009), modified to calculate assimilation based on Cc (An = f(Cc, Vcmax, Jmax, Rd)) through equations (1)–(5). Curves for ‘gm = infinity’ represent simulations run with no consideration for mesophyll diffusion conductance (An = f(Ci, Vcmax, Jmax, Rd)). Error bars represent the standard deviation from the mean. WUE is defined as the molar ratio of assimilation to transpiration. Daily values were assigned to 14 bins (n = 364). For each gm value, the following canopy integrated photosynthetic parameters were used: gm = 1, Vcmax = 35, Jmax = 70; gm = 0.2, Vcmax = 42.5, Jmax = 70; gm = 0.1, Vcmax = 51, Jmax = 70; gm = 0.05, Vcmax = 85, Jmax = 80). Please cite this article in press as: Keenan, T., et al., Soil water stress and coupled photosynthesis–conductance models: Bridging the gap between conflicting reports on the relative roles of stomatal, mesophyll conductance and biochemical limitations to photosynthesis. Agric. Forest Meteorol. (2010), doi:10.1016/j.agrformet.2010.01.008 G Model AGMET-4203; No of Pages 11 T. Keenan et al. / Agricultural and Forest Meteorology xxx (2010) xxx–xxx 6 Fig. 2. Water stressed simulated and FLUXNET measured responses of daily canopy net assimilation (An, g C m2 day1), and daily latent heat flux (LHF, W m2) to changes in soil water content at the Puechabon forest during 2002. Simulations use the coupled Farquhar BB-type model, on a Cc basis, embedded in the GOTILWA+ forest model (Keenan et al., 2008, 2009). Results from three simulations are presented, applying independently either: direct biochemical limitations to photosynthesis during water stress (BL, Eq. (6)), stomatal limitations to photosynthesis (SCL, Eq. (7)), or mesophyll conductance limitations to photosynthesis (MCL). Non-stressed mesophyll diffusion conductance (gm) was set at 0.1 mol m2 s1. Figure insets represent linear regressions between the measured and predicted variables (BL: An r2 = 0.92, LHF r2 = 0.65; SCL: An r2 = 0.7, LHF r2 = 0.69; MCL: An r2 = 0.75, LHF r2 = 0.52 (n = 77)). 1, Figs. 2 and 3), but the simulation of water fluxes slightly improved. 3.3. Long term comparison of approaches We tested the two effective modelling approaches (1: the application of BL, 2: the application of CL with MCL > SCL) against five years of flux data for the period from 2001 to 2005 at Puechabon forest (data not used for the calibration of the response functions). Both model approaches proved effective at capturing the seasonal effect of soil water stress on CO2 and water fluxes during the five year period (Fig. 5). Simulations with the CL (with MCL > SCL) approach and the BL approach explained 78% and 79% of the observed variance in canopy CO2 fluxes, respectively. This was confirmed by similar values of the Root Mean Squared Error (RMSE) statistic over the period, of 1.54 and 1.49, respectively. This was not true for the simulated latent heat flux. The BL approach achieved a higher correlation to the data (r2 = 0.75 vs. 0.71) but did not perform as well as the CL (with MCL > SCL) approach when considering the RMSE (17.1 vs. 14.8). The CL approach performed markedly better than the BL approach at simulating water fluxes for 2001, 2004 and 2005, which were the years which received the least precipitation (2001: 847 mm; 2004:705 mm; 2005: 875 mm; 5 year average: 966 mm). 4. Discussion A common approach to modelling stomatal conductance is to assume a linear relationship with leaf- or canopy-level photosynthesis (Wong et al., 1979), the leaf surface concentration of CO2, and relative humidity or vapour pressure deficit, the so-called ‘‘Ball-Berry’’ (BB) and ‘‘Ball-Berry-Leuning’’ (BBL) parameterizations (Ball et al., 1987; Leuning et al., 1995). Such assumptions underpin the coupling of water and CO2 cycles in many processbased ecosystem models, but water stress induced changes in conductance-photosynthesis relationships are as yet poorly understood. The effect of water stress on plant photosynthesis and stomatal conductance has been widely studied (Wilson et al., 2000; Chaves et al., 2002; Grassi & Magnani, 2005), but there is little consensus as to those processes governing responses over seasonal timescales (Loreto & Centritto, 2008; Warren, 2008a). Recent studies have shown that ‘non-stomatal’ limitations remove the need for stomatal limitations when modelling drought affects on coupled carbon-water photosynthesis models (Rambal et al., 2003; Reichstein et al., 2002, 2003; Keenan et al., 2009), due to the linear relation between photosynthetic demand and stomatal conductance, and are supported by reported changes in photosynthetic potential in the field (e.g., Xu and Baldocchi, 2003). Such results are controversial, as they suggest that stomatal conductance responses are not necessary for plant function under long term seasonal water stress events. There is no clear understanding of the processes responsible for such BL, though many different possibilities highlighted in the literature, such as enzyme deactivation (Tezara et al., 1999; Lawlor & Cornic, 2002), activity of aquaporins (Flexas et al., 2004; Kaldenhoff et al., 2008; Miyazawa et al., 2008), photosynthetic inhibition due to high temperatures (Haldimann & Feller, 2004), denitrogenisation (Grassi & Magnani, 2005), among many other possible mechanisms (e.g., Chaves et al., 2002; Lawlor & Cornic, 2002; Bota et al., 2004). It is well known that the stomata react to changes in soil water availability (e.g., Jones, 1973; Cornic, 2000; see Lawlor & Cornic, 2002 for a review). Stomata play a fundamental role in maintaining the water balance of the leaf, as water reserves in leaves and stems are very small when compared to the amount of water transpired, and thus could be quickly dehydrated in the absence of fast mechanisms, such as stomatal closure, to limit water loss (Slatyer, 1967). The effect of such stomatal closure is most commonly observed in the mid-day decline in stomatal conductance due to decreasing leaf water potential. This is suggested to limit photosynthetic activity through reducing Ci. Such short-term responses are, in theory, essential to conserving the plant hydraulic balance. There is evidence that water stress impairs mesophyll metabolism (Chaves, 1991; Lawlor & Cornic, 2002; Flexas et al., 2008). This has been linked to the hardening of cell walls and the increase in cell wall lignification in response to hydraulic signals (Escudero et al., 1992; Sobrado, 1992; Chazen and Neumann, 1994; Please cite this article in press as: Keenan, T., et al., Soil water stress and coupled photosynthesis–conductance models: Bridging the gap between conflicting reports on the relative roles of stomatal, mesophyll conductance and biochemical limitations to photosynthesis. Agric. Forest Meteorol. (2010), doi:10.1016/j.agrformet.2010.01.008 G Model AGMET-4203; No of Pages 11 T. Keenan et al. / Agricultural and Forest Meteorology xxx (2010) xxx–xxx Fig. 3. Water stressed simulated and FLUXNET derived responses of daily canopy water use efficiency (WUE, mmol mmol1) to changes in soil water content at the Puechabon forest in 2002. Simulations use the coupled Farquhar BB-type model, on a Cc basis, embedded in the GOTILWA+ forest model (Keenan et al., 2008, 2009). Results from three simulations are presented, applying independently either: direct limitations to photosynthesis during water stress (Vcmax/Jmax Restrictions), stomatal limitations to photosynthesis (gs Restrictions), or mesophyll conductance limitations to photosynthesis (gm Restrictions). Mesophyll diffusion conductance (gm) was set at 0.1 mol m2 s1. Figure insets represent linear regressions between the FLUXNET estimated and the simulated WUE (BL: r2 = 0.25; SCL: r2 = 0.06; MCL: r2 = 0.25 (n = 77)). Chazen et al., 1995; Henry et al., 2000), but could also be related to modifications in the permeability of membranes on the diffusion pathway from the intercellular spaces to the sites of carboxylation (Miyazawa et al., 2008). Strong responses have been reported in long term drought cycles of varying length and severity, with the mesophyll response becoming progressively more important with increasing water stress (e.g., Flexas et al., 2002; Warren & Adams, 2004; Monti et al., 2006; Galmés et al., 2007; Peeva & Cornic, 2009). Any changes in mesophyll conductance during periods of low soil water availability could potentially play an important role in controlling photosynthetic responses to water stress (Jones, 1973; Flexas et al., 2008). Unfortunately, to date there are no measurements of mesophyll conductance available at the Puechabon site. More measurement campaigns are badly needed in order to verify the results presented in this study. We have shown that the inclusion of mesophyll conductance could bridge the gap between our current understanding gained from field and model experiments (e.g., Reichstein et al., 2002; Xu 7 & Baldocchi, 2003; Keenan et al., 2009, 2010), and our functional understanding of leaf responses to water stress. The hypothesis that biochemical limitations are sufficient to accurately model CO2 and water fluxes (without any conductance limitations) has been confirmed (as in Reichstein et al., 2002; Keenan et al., 2009), and it has been shown that stomatal conductance limitations alone inevitably overestimate water use efficiency, and therefore, can effectively simulate water fluxes during water stressed periods but overestimate CO2 fluxes. Stomatal conductance limitations become effective at modelling CO2 and water fluxes only when combined with mesophyll conductance limitations, and vice versa, suggesting a close relation between the two (Flexas et al., 2008), and supporting previous suggestions of a joint role in regulating photosynthesis during periods of water stress (Grassi & Magnani, 2005). Finite mesophyll conductance affects estimates of the maximum carboxylation velocity, Vcmax, and their interpretation. Most published estimates of Vcmax, and its responses to soil water stress, will therefore underestimate the true Vcmax by not considering the draw-down from Ci to Cc, and may potentially assign declines in assimilation rates due to changes in gm during water stress to declining photosynthetic potential. To the knowledge of the authors no published study, either in the field or model based, which reported strong declines in photosynthetic potential during drought periods, has taken into account the possible effects of a soil water stress responsive gm. This does not suggest the exclusion of the possibility of biochemical limitations under stronger water stresses. Metabolic adjustments can take many forms, and may include the reduction of enzymes necessary for RuBP regeneration and activity (Maroco et al., 2002), reduced nitrate reductase activity (as an indicator of nitrate utilisation) (Smirnoff and Stewart, 1985), and the reduction of sucrose phosphate synthase (Vassey & Sharkey, 1989; Vassey et al., 2006). More field campaigns in ecosystems which are subject to seasonal cycles of water stressed periods will be necessary to improve our understand of the relative roles of each limitation. The representation of CO2 flux responses to drought often varies depending on the model applied, as it is a function of soil hydrology (with different approaches: single bucket soil module, two layer or multi-layer model), soil structure, forest structure and biogeochemistry assumptions. For example, the sensitivity to drought has been shown to be higher in models with a two layer soil hydrology model, and differences in soil structure and hydrology lead to differences in evapotranspiration calculations (Vetter et al., 2008). It has been assumed in this study that the eco-physiological state of the forest is well described in the model, as has been validated through previous applications of the model platform at this site (Keenan et al., 2008, 2009). gm strongly varies both among and within species (Ethier & Livingston, 2004; Flexas et al., 2008; Niinemets et al., 2009a; Warren, 2008a), and has been shown to be affected by a large range of environmental and physiological factors (see Flexas et al., 2008 for a full review), and demonstrate both fast (Flexas et al., 2007) and slow (Fila et al., 2006) responses. It has been demonstrated to change during leaf development (Miyazawa & Terashima, 2001), with nutrient availability (Warren, 2004), with available radiation (Niinemets et al., 2006), leaf temperature (Bernacchi et al., 2002), salinity (Loreto et al., 2003), ambient CO2 concentrations (Flexas et al., 2007) and to be related to soil water availability (Flexas et al., 2002, 2004; Warren, 2004, 2008a; Grassi & Magnani, 2005). This complicates the inclusion of a process based description of a dynamically variable and ecophysiological dependent gm in current photosynthesis models. As yet, it is not clear as to which factors have the largest effect on gm variability, and there is not sufficient physiological information to allow for a reliable estimation of a variable gm in process based models. Please cite this article in press as: Keenan, T., et al., Soil water stress and coupled photosynthesis–conductance models: Bridging the gap between conflicting reports on the relative roles of stomatal, mesophyll conductance and biochemical limitations to photosynthesis. Agric. Forest Meteorol. (2010), doi:10.1016/j.agrformet.2010.01.008 G Model AGMET-4203; No of Pages 11 8 T. Keenan et al. / Agricultural and Forest Meteorology xxx (2010) xxx–xxx Fig. 4. Water stressed simulated (applying combined conductance limitations: CL) and FLUXNET measured responses of canopy daily net assimilation (An, g C m2 day1), and daily latent heat flux (LHF, W m2) to changes in soil water content at the Puechabon forest during 2002. Simulations use the coupled Farquhar BB-type model, on a Cc basis, embedded in the GOTILWA+ forest model (Keenan et al., 2008, 2009). Results from three simulations to test CL are presented, applying either: (a) equal limitations to stomatal conductance and mesophyll conductance during water stress (SCL = MCL), (b) stronger stomatal limitations than mesophyll conductance limitations (SCL > MCL), or (c) stronger mesophyll conductance limitations than stomatal conductance limitations (MCL = SCL). Non-stressed mesophyll diffusion conductance (gm) was set at 0.1 mol m2 s1. Figure insets represent linear regressions between the measured and predicted variables (a) An r2 = 0.47, LHF r2 = 0.73; (b) An r2 = 0.43, LHF r2 = 0.65; (c) An r2 = 0.81, LHF r2 = 0.73 (n = 77)). Few studies have included gm in photosynthesis models. Those that have, most often assume a fixed value of mesophyll conductance (e.g., Williams et al., 1996), or varied gm based on selected factors such as intercepted radiation, average air temperature, or leaf nitrogen content (e.g., Hoff et al., 2002; Ohsumi et al., 2007). Recent efforts have focused on reported correlations between gm and gs (e.g., Ohsumi et al., 2007; Cai et al., 2008). Such correlations, however, are subject to large variations (Niinemets & Sack, 2006; Warren & Adams, 2006; Flexas et al., 2008), and potentially not physiologically justified. Maximum values of gm are inherently constrained by leaf structure, e. g. sclerophytic leaves have lower gm, mesophytic leaves have higher (Terashima et al., 2006; Flexas et al., 2008; Warren, 2008a; Evans et al., 2009; Niinemets et al., 2009a), which may be an effective manner by which to include gm in photosynthesis models. Largescale models (e.g., Morales et al., 2005; Jung et al., 2007; Sitch et al., 2008) in particular, due to their characteristic simplification of plant functional type groupings, may benefit from such an approach. Although there are huge uncertainties regarding the driving factors responsible for variations in gm we have shown that the simple inclusion of a water stress responsive gm can help close the gap between conflicting reports on the role of different limitations in controlling CO2 and water fluxes from forest canopies during water stressed periods. The inclusion of gm did not improve our ability to model in ecosystems subject to seasonal cycles of water stress, but much of the remaining variability between measured and modelled CO2 and water fluxes may be explained, as new information accumulates in the future, through the inclusion of a dynamically variable gm. 5. Conclusions Fig. 5. Simulated and FLUXNET responses of canopy daily net assimilation (An, g C m2 day1), and daily latent heat flux (LHF, W m2) for the five year period from 2001 to 2005 at Puechabon forest using the GOTILWA+ model (Keenan et al., 2008, 2009). Two simulations, differing in their response to soil water stress, are compared: (1) Soil water stress affects both conductance limitations (CL), with MCL stronger than SCL (Blue, long dashed line), (2) Soil water stress directly affects Vcmax and Jmax (BL: Red, short dashed line). Non-stressed mesophyll diffusion conductance (gm) was set at 0.1 mol m2 s1. Right panel figures represent linear regressions between the measured and predicted variables (CL (MCL > SCL): An r2 = 0.78, LHF r2 = 0.72; BL: An r2 = 0.79; LHF r2 = 0.76 (n = 1825)) (For interpretation of the references to color in this figure legend, the reader is referred to the web version of the article.). This work was carried out in response to the recent calls for the inclusion of mesophyll conductance in leaf photosynthesis models (e.g., Bernacchi et al., 2002; Flexas et al., 2002; Long & Bernacchi, 2003; Ethier & Livingston, 2004; Manter & Kerrigan, 2004; Sharkey et al., 2007; Keenan et al., 2010; Niinemets et al., 2009b), due to an increased number of reported findings on the role of mesophyll conductance in the regulation of photosynthesis. It has allowed for a model based assessment of previous suggestions that biochemical limitations, stomatal conductance limitations and mesophyll conductance limitations play some role in the regulation of Please cite this article in press as: Keenan, T., et al., Soil water stress and coupled photosynthesis–conductance models: Bridging the gap between conflicting reports on the relative roles of stomatal, mesophyll conductance and biochemical limitations to photosynthesis. Agric. Forest Meteorol. (2010), doi:10.1016/j.agrformet.2010.01.008 G Model AGMET-4203; No of Pages 11 T. Keenan et al. / Agricultural and Forest Meteorology xxx (2010) xxx–xxx photosynthesis (Grassi & Magnani, 2005; Loreto & Centritto, 2008), depending on the degree of water stress encountered and the relevant time scales involved. This is the first time that each limitation has been tested on a canopy scale in an ecophysiological model, and shows that, with (and only with) the inclusion of mesophyll conductance, diffusive limitations can explain CO2 and water flux responses to seasonal changes in soil water availability. This helps in closing the gap between studies (both model and measurement based) which report dominant roles of biochemical changes under water stressed conditions and those which maintain stomatal conductance limitations as the main actor. It is expected that the future development of a dynamic model for mesophyll conductance which incorporates sensitivity to nonwater stress related drivers, and its integration into coupled photosynthesis–conductance models will improve our ability to model CO2 and water fluxes from terrestrial ecosystems both in well watered and water stressed periods. Acknowledgments This study was funded through GREENCYCLES, the Marie-Curie Biogeochemistry and Climate Change Research and Training Network (MRTN-CT-2004-512464) supported by the European Commissions Sixth Framework program. Further support from the CCTAME (Climate Change-Terrestrial Adaptation and Mitigation in Europe, FP7 212535) project and the Consolider Montes project (CSD2008-00040) is also acknowledged. The authors would like to thank Serge Rambal and highly commend all the FLUXNET investigators whose data has contributed to the work discussed here. References Aber, J.D., Federer, C.A., 1992. 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Please cite this article in press as: Keenan, T., et al., Soil water stress and coupled photosynthesis–conductance models: Bridging the gap between conflicting reports on the relative roles of stomatal, mesophyll conductance and biochemical limitations to photosynthesis. Agric. Forest Meteorol. (2010), doi:10.1016/j.agrformet.2010.01.008
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