Tree Physiology 28, 529–536 © 2008 Heron Publishing—Victoria, Canada Persisting soil drought reduces leaf specific conductivity in Scots pine (Pinus sylvestris) and pubescent oak (Quercus pubescens) FRANK J. STERCK,1,2 ROMAN ZWEIFEL,3 UTE SASS-KLAASSEN1 and QUMRUZZAMAN CHOWDHURY1 1 Forest Ecology and Forest Management Group, Wageningen University, P.O. Box 47, 6700 AA Wageningen, The Netherlands 2 Corresponding author ([email protected]) 3 Swiss Federal Institute for Forest, Snow and Landscape Research (WSL), Birmensdorf, Switzerland Received January 31, 2007; accepted July 6, 2007; published online February 1, 2008 Summary Leaf specific conductivity (LSC; the ratio of stem conductivity (KP ) to leaf area (AL )), a measure of the hydraulic capacity of the stem to supply leaves with water, varies with soil water content. Empirical evidence for LSC responses to drought is ambiguous, because previously published results were subject to many confounding factors. We tested how LSC of similar-sized trees of the same population, under similar climatic conditions, responds to persistently wet or dry soil. Scots pine (Pinus sylvestris L.) and pubescent oak (Quercus pubescens Willd.) trees were compared between a dry site and a wet site in the Valais, an inner alpine valley in Switzerland. Soil water strongly influenced AL and KP and the plant components affecting KP, such as conduit radius, conduit density and functional sapwood area. Trees at the dry site had lower LSC than trees with the same stem diameter at the wet site. Low LSC in trees at the dry site was associated with a smaller functional sapwood area and narrower conduits, resulting in a stronger reduction in KP than in AL. These observations support the hypothesis that trees maintain a homeostatic water pressure gradient. An alternative hypothesis is that relatively high investments in leaves compared with sapwood contribute to carbon gain over an entire season by enabling rapid whole-plant photosynthesis during periods of high water availability (e.g., in spring, after rain events and during morning hours when leafto-air vapor pressure deficit is small). Dynamic data and a hydraulic plant growth model are needed to test how investments in leaves versus sapwood and roots contribute to transpiration and to maximizing carbon gain throughout entire growth seasons. Keywords: Huber value, leaf area, soil water potential, stem conductivity. Introduction Trees adjust the functional balance among organs and tissues responsible for water acquisition (fine roots), transport (sapwood) and transpiration (leaves) (Cannell and Dewar 1994). Leaf specific conductivity (LSC; the ratio of stem conductivity to leaf area (KP /AL ); abbreviations and units are listed in Table 1) is considered a measure of hydraulic capacity of the stem to supply leaves with water (Tyree and Zimmermann 2002). According to physical principles, KP should increase linearly with sapwood cross-sectional area, conduit density within sapwood and the fourth power of the radius of the conduits. If conduit properties are constant, LSC scales directly with the Huber value (H; sapwood area divided by leaf area (AS /AL )). Although modeling studies predict an increase in LSC or H in response to drought (Whitehead et al. 1984, Magnani et al. 2002), few empirical studies have confirmed these predictions (Mencuccini and Bonosi 2001, Cherubini et al. 2003) and some have shown the reverse pattern (Panek 1996, Vander Willigen and Pammenter 1998). These studies focused on the effects of the vapor pressure deficit between leaves and air (VPD), but the results may have been confounded by environmental, genotypic or size differences across sites. Most empirical studies showing that LSC or H increases with soil drying have investigated effects of short-term drought pulses (Irvine et al. 1998) or drainage pulses (Ewers et al. 2000), rather than persistent soil drought. An exception is the study by Addington et al. 2006 which found that, in Pinus palustris Mill., H was lower at the site with persistently drier soil, but this was mainly explained by variation in tree size across sites. From the cited studies, it can be concluded that the observed responses of LSC and H to drought are often confounded by ontogenetic responses, genotypic variation, site dynamics, climate factors, short-term versus long-term structural responses or interspecific differences. In this study, we explored LSC responses to persistent soil drought by comparing tree populations that experience different soil water availabilities (wet site versus dry site). By looking at the same tree population, we consider only phenotypic responses to soil drought and exclude strong microclimatic (e.g., VPD) effects. We analyzed how morphological plant components contribute to the overall drought response in LSC (Figure 1). We predicted that KP decreases in response to increasing soil drought because of a smaller AS and smaller conduit sizes (R) (Figure 1A; cf. Eilmann et al. 2006). Although 530 STERCK, ZWEIFEL, SASS-KLAASSEN AND CHOWDHURY Table 1. Symbols and abbreviations used in the Equations. For statistical analyses and representation in figures and tables, other units may be used. The entire sapwood was considered conductive in Scots pine (Pinus sylvestris), but only the outer annual growth ring of the sapwood was considered conductive in pubescent oak (Quercus pubescens). Code Description Units AL AS AEW ALW Dstem D DEW DLW KP KPEW KPLW R REW RLW LSC DS Total leaf area Functional sapwood cross-sectional area AS in earlywood AS in latewood Stem diameter 50 cm above stem base Conduit density D in early wood sapwood D in late wood sapwood Potential stem conductivity KP of earlywood KP of latewood Hydraulic conduit radius R in the earlywood R in the latewood Leaf specific conductivity (KP /AL) Drought-induced stress H η ρw k ψ gs h Huber value (AS /AL) Viscosity of water at 20 °C Density of water at 20 °C Sapwood permeability Pressure Stomatal conductance Length from roots to leaves m2 m2 m2 m2 m m– 2 m– 2 m– 2 kg m MPa – 1 s – 1 kg m MPa – 1 s – 1 kg m MPa – 1 s– 1 m m m kg m –1 MPa – 1 s – 1 0 for wet site; 1 for dry site – Pa s kg m – 3 kg m MPa – 1 s – 1 MPa mol m – 2 s – 1 m the smaller conduit size may be compensated by a higher conduit density (D), the fourth power contribution of R to KP, according to Hagen-Poiseuille principles, will result in a net decrease in KP. Total AL, the other main component of LSC (Figure 1B), is predicted to decrease in response to soil drying because of previous-year limitations in resource acquisition and bud formation (Zweifel et al. 2006). Specifically, we tested two alternative hypotheses by comparing Scots pine (Pinus sylvestris L.) and pubescent oak (Quercus pubescens Willd.) trees growing on dry slopes with trees growing along irrigation channels on the same slope in the Valais: (1) LSC increases as soil dries because of a greater effect on AL than on KP (Figure 1B); and (2) LSC decreases as soil dries because of a greater effect on KP than on AL. Materials and methods Study site The study was carried out on a south-facing slope in the Valais, Salgesch, Switzerland (46°19′27″ N, 7°34′40″ E) in the summer of 2005. The area receives about 600 mm annual precipitation, distributed throughout the year (Zweifel et al. 2005). Mean monthly temperature varies from –1 °C in January to Figure 1. A conceptual model of relationships among plant traits. Single-headed arrows denote direct effects, and double-headed arrows denote correlations. (A) Effects of drought-induced stress (DS) on functional sapwood area (AS), conduit radius (R) and conduit density (D), and in turn, the contributions of these components to potential stem conductivity (KP ). (B) Effects of DS on total leaf area (AL) and KP and, in turn, of the contributions of AL and KP to leaf specific conductivity (LSC). Signs adjacent to arrows indicate the expected relationships. 19 °C in July. The soil is 10–30 cm deep and classified as a rendzic leptosol on solid rock limestone (Rigling et al. 2002). The main tree species are pubescent oak (Quercus pubescens) and Scots pine (Pinus sylvestris), henceforth referred to as oak and pine. To test our hypotheses we compared trees on a dry slope (dry site) with trees along an irrigation channel on the same slope (wet site), on the assumption that the sites differed only in soil water availability. Field experiment We selected 10 trees of each species (stem diameter 3–18 cm; measured 50 cm above the stem base) from the dry site, and another 10 trees of each species growing within 2 m of an irrigation channel (wet site). Selected trees were a minimum of 50 m from each other to reduce pseudo-replication effects. The 40 trees occurred at a maximum distance of 500 m from one another, and were selected within a narrow altitudinal range (950–1000 m) to avoid confounding effects of climate. The following variables were measured in the field: stem diameter at 50 cm aboveground (Dstem); tree and lowest branch heights; crown radius in eight directions; and the number of apices of leaf-bearing shoots. For each tree, two cores were taken 50 cm above the stem base, with an increment corer (Suunto, Finland), and prepared for dendrochronological and wood anatomical analyses. To improve the contrast between cell lumen and cell walls, the core samples were soaked in 10% NaOH, air dried, and the surface rubbed with chalk to fill the conduit lumens. Ring width, earlywood width and late- TREE PHYSIOLOGY VOLUME 28, 2008 DROUGHT AND LEAF SPECIFIC CONDUCTIVITY wood width were measured over the whole radius with the LINTAB system and Time Series Analysis and Presentation software (TSAP, Rinntech, Heidelberg, Germany). Heartwood and sapwood were demarcated on the cores; a 1:1 (v/v) mix of sulfuric acid:sodium nitrate (50%) was applied to improve the contrast for pine (Cummins 1972). Conduit radius was measured for early- and latewood in 5 randomly selected conduits in the earlywood and 5 in the latewood of each of the last seven consecutive rings, using UTHSCSA Image Tool software v.3.0 (http://ddsdx.uthscsa.edu/dig/itdesc.html). The same software was used to measure conduit density. Five randomly selected branches were harvested per tree. The apices of these branches were counted. Leaves were harvested and dried, and leaf dry mass determined. The product of leaf mass and the ratio of number of apices in the whole tree to number of apices in the five branches gave an estimate of total leaf mass. We also measured leaf area of 50 leaves, and calculated specific leaf area (leaf area:leaf mass ratio) to predict AL from the product of total leaf mass and specific leaf area. Hydraulic parameter calculations For each tree, the functional balance between water transport in the stem and transpiration of water through the leaf surface area was expressed by H and LSC. In this study, we defined AS as the actual sapwood area for Scots pine (Èermák et al. 1992) and the outermost ring area for pubescent oak (Hinckley et al. 1979, Bréda and Granier 1996, Tognetti et al. 1998, Nardini and Pitt 1999, Barbaroux and Bréda 2002, Domec and Gartner 2002, Cherubini et al. 2003, Zweifel et al. 2006 ). We calculated KP from the potential conductivity in earlywood (KPEW) and latewood (KPLW): K P = K PEW + K PLW (1) We calculated KPEW and KPLW from the hydraulic conduit radius (REW or RLW, respectively), conduit density (DEW or DLW, respectively) and sapwood area (AEW or ALW, respectively), with the Hagen-Poiseuille equation. The hydraulic conduit radius R was calculated for early- and latewood separately as: 1 ⎛1 n ⎞4 R = ⎜ ∑ ri4 ⎟ ⎝ n i =1 ⎠ (2) 531 where ri is the ith conduit of n (n = 70) measured conduits in the earlywood (REW) and latewood (RLW). Parameters AEW and ALW refer to the areas of the sapwood (in early and latewood, respectively) in pine, and of the outer ring in oak (cf. Table 1). K PEW = π 4 ρw AEW DEW REW 8n (3) K PLW = π 4 ρw ALW DLW RLW 8n (4) where η is viscosity of water (1.002 × 10 – 3 Pa s at 20 °C) and ρw is density of water (998.2 kg m – 3 at 20 °C). Although the calculations of KP, KPEW and KPLW overestimate actual sapwood conductivity, they serve as precise comparative measures of stem conductivity within species (Steppe and Lemeur 2007). Results Although pine trees had a smaller AS at the dry site than at the wet site, they had more, and consequently, narrower rings in the sapwood (Figure 2). Thus, pines at the dry site seemed to compensate for slow radial stem growth by delayed conversion of sapwood into heartwood. In oaks, AS was assumed to be equivalent to the outer ring, which was larger in trees at the wet site than at the dry site. Although H decreased with stem size, it hardly differed between the sites (Figure 3). Leaf specific conductivity in oak was only a tenth that in pine. As shown in Figure 3, LSC did not change with stem diameter in pine, but declined with stem diameter in oak (Figure 3). Except for the smallest oaks, LSC was lower at the dry site than at the wet site in both species. Path-analysis showed that the negative effect of AL on LSC was compensated by the positive effect of KP (see path-coefficients: –0.90 versus 1.08 in oak (Figure 4A), and –1.32 versus 1.46 in pine (Figure 4B)), and that a stronger decline in KP than in AL at the dry site accounted for the site response in LSC (see Figure 4: –0.77 versus –0.33 in oak, and –0.64 versus –0.17 in pine; also see Figures 3E–H). Although AS was smaller in trees at the dry site than at the wet site, particularly in pine, the difference was insufficient to account for the observed site Figure 2. Comparison of (A) total number of rings in the sapwood and (B) mean ring area with stem diameter 50 cm above stem base (Dstem) for Pinus sylvestris trees at the dry (䊊) and wet (䊉) sites in the Valais, Switzerland. TREE PHYSIOLOGY ONLINE at http://heronpublishing.com 532 STERCK, ZWEIFEL, SASS-KLAASSEN AND CHOWDHURY Figure 3. Effects of site (drought-induced stress; DS) on functional relationships in trees differing in stem diameter Dstem (n = 10) in Quercus pubescens and Pinus sylvestris trees at the dry (䊊) and wet (䊉) sites. (A, B) Huber value (H), (C, D) leaf specific conductivity (LSC), (E, F) total leaf area (AL) and (G, H) potential conductivity (KP ). If regression analysis indicated significant interaction effects of (DS × Dstem ), regressions are shown for each site separately. Otherwise, ANCOVA was performed to distinguish between the effects of DS and Dstem (see Table 1 for parameter codes, and Table 2 for statistics). variation in LSC (see Figure 2). The site effects on REW and DEW mirrored one another (see opposite signs of path-coefficients in Figure 5), because smaller conduits allow for higher densities. In turn, however, REW had a much greater effect on KP than did DEW, because KP increased with REW to the 4th power (cf. Equation 3). Because of the small values of RLW and ALW, the latewood contributions to LSC were less than the early wood contributions in both species. Taken together, these results indicate that the combined effects of drought on KP, which were mediated by AS and R, and the rather weak effect on AS resulted in lower LSC at the dry site than at the wet site for both species. Discussion Growth Trees at the dry site produced fewer leaves and less wood than trees at the wet site, as indicated by the smaller AL, narrower annual growth rings and smaller AS. Lower productivity at the dry site than at the wet site was expected, because foliage of trees on a dry site is characterized by limited stomatal conductance (gs ), lower carbon gain, which reduces shoot and leaf production, and lower cell turgor, which reduces radial wood growth (Tyree 2003, Gallé 2006, Zweifel et al. 2006, 2007). In a study with Pinus palustris, such drought-driven limitations TREE PHYSIOLOGY VOLUME 28, 2008 DROUGHT AND LEAF SPECIFIC CONDUCTIVITY 533 Table 2. Summary of regression analysis of the effects of stem diameter (Dstem ) and drought-induced stress (DS) on the Huber value (H; sapwood area:leaf area (AS /A L )), specific leaf conductivity (LSC), and underlying morphological components in Quercus pubescens and Pinus sylvestris trees. For Q. pubescens, the interaction effect of Dstem × DS was significant, and the model was run for individuals from each site separately. Log-log transformed values were used in the regression model: log10(LSC) = a + blog10(Dstem ) + cDS + d(log10(Dstem) × DS), where DS is a dummy variable (wet site = 0, dry site = 1). Effects of Dstem and DS are shown by b and c values. Intercept value a is not shown. Significance of the coefficient is indicated as: *, P < 0.05; **, P < 0.01; ***, P < 0.001; nr, not relevant for single factor regressions on Dstem; and ns, not significant (P > 0.05). Dstem effect = b DS effect = c Quercus pubescens H wet H dry LSC wet LSC dry KP AL AS REW DEW –0.56 * –1.30 *** – –1.44 *** ns 1.27 *** 0.36 * ns ns nr nr nr nr –0.53 *** –0.18 *** –0.38 *** –0.10 *** 0.16 *** Pinus sylvestris H LSC KP AL AS REW DEW –0.37 ** – 1.43 *** 1.80 *** 1.44 *** ns ns – –0.48 *** –0.64 *** –0.16 ** –0.18 *** –0.17 *** 0.17 *** Figure 4. Path-analysis. Effects of site (drought-induced stress, DS) and stem diameter (Dstem) on total leaf area (AL ) and potential stem conductivity (KP) and, in turn, the contributions of AL and KP to leaf specific conductivity (LSC) in (A) Quercus pubescens and (B) Pinus sylvestris. Path-coefficients (standardized regression coefficients) along single-headed arrows refer to direct effects, and correlation coefficients along double-headed arrows refer to correlations. Significance of effects and correlations are indicated as: **, P < 0.01; and ***, P < 0.001. in production were not observed, because AS was similar across sites and AL was larger at the dry site (Addington et al. 2006). Possibly, the higher annual precipitation in that study area compared with our site (1310 versus 600 mm) reduced the severity of soil drought. The low productivity of our study trees at the dry site suggests that the soil drought was more severe. Wood anatomy Soil water strongly influenced AL and KP and the wood characteristics affecting KP. As expected, pines and oaks had considerably narrower conduits in both early- and latewood and higher conduit densities at the dry site. This accords with the idea that cell expansion rate and cell size are controlled by turgor pressure (Hsiao and Avecedo 1974, Steppe et al. 2006), and that cell expansion rate and ultimate cell size decrease with decreasing water availability (Sass and Eckstein 1995, Villar-Salvador et al. 1997, Zweifel et al. 2006). Dendrochronological studies have demonstrated that time series of conduit size correlate positively with corresponding precipitation (e.g., Sass and Eckstein 1995). However, Eilmann et al. (2006) reported that latewood conduit size decreased with increasing precipitation in trees at our study site. This may have Figure 5. Path-analysis. Effects of site (drought-induced stress, DS) on functional sapwood area (AS), conduit radius (R) and conduit density (D) and, in turn, the contributions of these components to potential stem conductivity (KP) in (A) Quercus pubescens and (B) Pinus sylvestris. Path-coefficients (standardized regression coefficients) along single-headed arrows refer to direct effects, and correlation coefficients along double-headed arrows refer to correlations. The relationships are shown for the earlywood traits (AS, R and D), because the latewood contributions to leaf specific conductivity were less in both species. Significance of effects and correlations are indicated as: *, P < 0.05; and ***, P < 0.001. TREE PHYSIOLOGY ONLINE at http://heronpublishing.com 534 STERCK, ZWEIFEL, SASS-KLAASSEN AND CHOWDHURY resulted from limited cambial activity at the dry site in the summer, a delayed response to earlier conditions or multiple confounding factors (see Cherubini et al. 2003). In our study, the persistent soil drought resulted in narrower latewood conduits, as expected in response to a likely drought-driven decline in turgor in trees at the dry site (Villar-Salvador et al. 1997, Zweifel et al. 2005). Potential stem conductivity We calculated KP based on theoretical principles, as expressed by the Hagen-Poiseuille equation (see Equations 2–4). We assumed that the conductive cross-sectional area equaled the total sapwood area for pine (e.g., Whitehead et al. 1984) and the area of the last ring for oak (cf. Bréda and Granier 1996). The higher conductivity for pine than for oak agrees with ecophysiological information for trees from the same site (Zweifel et al. 2007). The potential conductivity may have been underestimated for oak, because the early wood in some older rings may have contributed to sap flow (Poyatos et al. 2007a), which was unaccounted for in our calculations. For both species, potential conductivity, may have been higher than actual conductivity because it takes no account of end wall resistances (Sperry et al. 2005) and vulnerability to cavitation (Maherali et al. 2004). Some field studies derive conductivity from measurements of sap flow and microclimate (Zweifel et al. 2005), but cannot relate the conductance to actual functional sapwood area. When KP is quantified for xylem sections exposed to controlled water pressure gradients in the laboratory (Cavender-Bares and Holbrook 2001), assumptions about the conductive xylem area are needed to predict conductance for trees under field conditions. It may be reasonable to assume that the entire xylem cross-sectional area contributes to water transport in beech (Fagus sylvatica L.) and oak (Quercus robur L.) seedlings (Steppe et al. 2006). In studies of beech and oak seedlings, the actual conductivities match the theoretical prediction, i.e., assuming the entire xylem cross section contributes to stem conductivity multiplied by a species-specific factor with a value of less than 1.0 (Steppe and Lemeur 2007). This finding suggests that the potential conductivity, as calculated from the Hagen-Poiseuille equation, can be used for comparative studies within species (cf. Sperry et al. 2005). Leaf specific conductivity For both pines and oaks, LSC was lower at the dry site than at the wet site. Magnani et al. (2002) predicted the reverse pattern, but cautioned that the empirical evidence for this prediction was based on studies with large trees exposed to drought pulses for only a few years (e.g., Irvine et al. 1998), or to short irrigation pulses (e.g., Ewers et al. 2000). The observed increase in LSC in response to drought pulses reflects a sharp increase in leaf production and AL, but little change in wood production and AS. For trees growing under persistent dry conditions, we found the reverse pattern: a decline in LSC, indicating that trees favor allocation to leaves over allocation to radial growth, which accords with many empirical studies compar- ing trees along drought gradients (Panek 1996, Vander Willigen and Pammenter 1998), but not all (Mencuccini and Bonosi 2001). Addington et al. (2006) found a lower H in Pinus palustris in response to persistent soil drought; however, after controlling for differences in tree height between dry and wet sites, they concluded that the site effect on H was negligible. Thus, their findings for P. palustris are in agreement with the drought responses of H that we observed in P. sylvestris and, at least partially, with those we observed in Quercus pubescens. The large difference in LSC between trees at our dry and wet sites thus confirms that conduit properties significantly contributed to the observed drought responses in LSC, particularly in pine. In previous studies, drought-driven increases in LSC or H were usually related to higher VPD during periods of drought, and these effects were discussed in the context of the hydraulic model presented by Whitehead et al. (1984) (e.g., Poyatos et al. 2007b). Here we use the same model to discuss the effect of persisting soil drought on hydraulic architecture: AL c k ⎛ Δψ ⎞ = ⎜ ⎟ AS gs VPD ⎝ h ⎠ (5) where the constant c combines several variables that are weakly temperature dependent (Whitehead et al. 1984), Δψ/h is the pressure gradient (Δψ) measured over length (h) from roots to leaves, gsVPD is the transpiration demand and k is the permeability of the sapwood. Sapwood permeability may be related to conduit radius (R) and conduit density (D) according to the Hagen Poiseuille equation as: k ∝ DR4 (6) By dividing Equation 5 by k, we get an equation for the expected response of LSC: c ⎛ Δψ ⎞ 1 ∝ ⎜ ⎟ LSC gs VPD ⎝ h ⎠ (7) Although we distinguished between early- and latewood conductivities in our calculations, the general relationship is well described by Equation 7, which predicts that LSC increases with VPD and gs VPD. Such responses would contribute to homeostatic regulation of Δψ. Whitehead et al. (1984) suggested that H will be lower at a warmer and drier site than at a cooler and wetter site. The prediction that H and LSC (ASKP /AL ) are higher at the drier site assumes that k is similar across sites. However, site comparisons indicate that this is not the case for pines and oaks (cf. Eilmann et al. 2006). Permeability was lower for early- and latewood at the dry site, a difference that was at least partially compensated for the lower gs and gsVPD, assuming only minor differences in VPD between sites. This response in k limits the change in H in response to drought, which hardly differed between sites in either study species. Moreover, it may largely account for the reduction in LSC in response to drought. From this perspective, our results TREE PHYSIOLOGY VOLUME 28, 2008 DROUGHT AND LEAF SPECIFIC CONDUCTIVITY agree with the hydraulic model and suggest that a combined response in physiology (i.e., gs ) and plant structure (LSC and its components) contribute to acclimation of hydraulic architecture to soil drought (Martinez-Vilalta et al. 2004, Zweifel et al. 2006). This line of reasoning assumes constant conditions at the dry and wet sites. Drought, however, varies at many time scales including days, seasons and successive years (e.g., Zweifel et al. 2005, 2007). At these time scales, stomata close during dry periods (Zweifel et al. 2006), limiting carbon gain (Tyree 2003), implying that trees fix carbon mainly during wet periods when AL is the main limitation on carbon gain. Accordingly, we may expect that trees in arid areas, such as the Valais, favor carbon allocation to leaves rather than to radial growth, because a large AL is highly advantageous during wet periods. Furthermore, from a physiological perspective, low turgor in the cambium will reduce radial growth in arid areas (Steppe et al. 2006), whereas growth limitations due to low turgor are less severe during spring leaf expansion (Zweifel et al. 2006). The severe drought at our dry site may therefore limit wood production rather than leaf production. The resultant high resistances to water flow in trees at the dry site may be compensated, at least partially, by an ability to maintain sap flow at lower leaf water potentials (Zweifel et al. 2007). However, during severe drought, such as during the 2003 summer, sap flow may fall to zero, resulting in massive leaf loss and persistent low water flow (Zweifel et al. 2007), especially in oak. In conclusion, pines and oaks had a lower LSC at the dry site than at the wet site because of smaller AS, narrower conduits and a greater reduction in KP than in AL. The resultant low hydraulic capacity during dry weather may be compensated for by lower leaf water potentials, lower vulnerability to xylem cavitation and greater resource allocation to fine roots, but these features were not analyzed. We speculate that relatively high investments in leaves contributed to carbon gain over a whole season by enabling high rates of whole-plant photosynthesis during the wetter periods (e.g., in spring, after incidental rains and during morning hours). Dynamic data and a hydraulic plant growth model are needed to test how investments in leaves versus sapwood and roots (cf. 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