Study site, species, and design
The experiment was conducted in French Guiana at the Paracou experimental station (https://paracou.cirad.fr/website; 5° 16′ 26″ N, 52° 55′ 26″ W), which represents a lowland tropical rainforest (Gourlet-Fleury et al. 2004). The warm and wet tropical climate of French Guiana is highly seasonal due to the North–South movement of the Intertropical Convergence Zone. Mean (± SE) annual air temperature is 25.7 °C ± 0.1 °C and the mean annual precipitation is 3,102 mm ± 70 mm (data between 2004 and 2014; Aguilos et al. 2019). There is a dry season lasting from mid-August to mid-November, during which rainfall is < 100 mm month−1.
We sampled only dominant canopy trees, and only growing on terra firme. A total of 50 trees belonging to 18 species and 50 trees were sampled, with three trees per species for 14 species, and two trees per species for four species (Bocoa prouacensis, Iryanthera sagotiana, Moronobea coccinea, Qualea rosea). These 50 trees represent a subset of the sampling in Ziegler et al. (2019), for which stem embolism resistance was initially measured. The same dataset was used by Levionnois et al. (2020), who added data on leaf embolism resistance. Measurements of stem or leaf embolism resistance were particularly challenging for species for which data on only two individuals were available. Although several samples have been collected for a given species, only two vulnerability curves (VC) per species could be obtained (Ziegler et al. 2019; Levionnois et al. 2020). The studied species covered a broad phylogenetic diversity such that the main clades of the flowering plants were represented, i.e. magnoliids, rosids, and asterids. Branches were sampled by professional tree climbers.
We calculated desiccation time at the shoot level, with a shoot defined in the context of this study as an unbranched and leafy stem, with the largest possible number of leaves and with all nodes bearing a leaf. The traits necessary for calculating shoot desiccation time were measured as much as possible at the shoot level, except for stem embolism resistance and stem capacitance, which were measured further upstream, on older branch sections (~2 cm in diameter).
Stem embolism resistance
Stem embolism resistance was measured as the stem water potential inducing 50% and 88% loss of conductivity (P50,stem and P88,stem, respectively; MPa; Table 1). Sample collection was held between January and July 2017, with one 3-m-long canopy branch sampled per tree. Only sun-exposed branches were sampled, except for the understory species Gustavia hexapetala. Vulnerability curves were measured with the flow-centrifugation technique using a Cavi1000 system (DGMeca, BIOGECO lab, Gradignan, France). A detailed description of the methods and the data for each species were provided and discussed by Ziegler et al. (2019).
Table 1 List of traits, abbreviations, and formula when appropriate Leaf embolism resistance
Leaf embolism resistance was measured as the leaf water potential inducing 50% and 88% loss of conductivity, respectively (P50,leaf and P88,leaf respectively; MPa; Table 1). The field sampling was held between November 2018 and March 2019, on the same trees that were sampled for the measurements of stem embolism resistance. We generally sampled three trees per sampling day, during the morning and before solar midday, in order to avoid too negative leaf water potentials and potential native leaf embolism. Only sun-exposed branches were sampled as much as possible. One 1-m-long canopy branch was sampled per tree, with ~50 leaves or leaflets for the monitoring of water potentials, as described below. A second small branch was also sampled for bark conductance and morphological measurements, as described below. To measure leaf xylem embolism resistance, we relied on the optical light transmission method (Brodribb et al., 2016a, 2016b; https://www.opensourceov.org). For details about the method and data for each species of this study, we refer the reader to Levionnois et al. (2020).
Leaf pressure–volume curves
Stomatal closure is generally measured from the stomatal response curve to leaf water potential based on stomatal conductance measurements. However, Ψclosure and leaf water potential at leaf turgor loss point (Ψtlp; MPa; Table 1) are strongly related (Brodribb et al. 2003; Rodriguez‐Dominguez et al. 2016; Bartlett et al. 2016), leading to the possibility to use Ψtlp as a surrogate of Ψclosure (Martin‐StPaul et al. 2017). Ψtlp was measured by pressure–volume analysis using the bench drying technique (Koide et al., 1989). Pressure–volume measurements were based on the measurement of one leaf per tree. Before the branch used for the measurement of leaf embolism resistance was removed from water and plastic bags, one fully hydrated and healthy leaf was sampled. At regular intervals, leaf water potential was measured with a Scholander pressure chamber (Model 600, PMS), directly followed by the measurement of leaf mass with a precision balance (AB 204-S, Mettler Toledo). The different water potential and mass measurements were made to cover the range from 0.00 to −3.00 MPa (or more if necessary as the dynamic of water potential drop is generally clearly noticeable during measurement), with ca. 0.30 MPa intervals. Then, the leaf was scanned to measure leaf area, and dried for 3 days at 70 °C to measure leaf dry mass Ψtlp being the leaf water potential at the phase transition (Koide et al. 1989). The pressure–volume curve was also used to derive leaf capacitance after turgor loss Wtlp,leaf (mmol m−2 MPa−1; Table 1), since the plant water stock used for the calculation of tcrit is the water available in plant tissues after stomatal closure. Wtlp,leaf was calculated as the slope of the loss of leaf water mass according to leaf water potential for water potentials below Ψtlp, and divided by the leaf area.
Stem capacitance
Wood capacitance is negatively related to wood density (Scholz et al. 2011; Mcculloh et al. 2014; Jupa et al. 2016; Santiago et al. 2018). Santiago et al. (2018) recently measured branch wood capacitance at full-turgor (Wft,stem;kg m−3 MPa−1) across 14 tropical rainforest canopy tree species at the same site as this present study in Paracou, French Guiana. Santiago et al. (2018) found a linear relationship (R2 = 0.59) between Wft,stem and branch wood density (WD, g cm−3; Table 1), such as: Wft,stem = −930.93 * WD + 868.97. We used the estimation of wood capacitance as a proxy for whole stem capacitance. We are aware that the different stem tissues (pith, xylem, phloem, cortex) can exhibit different capacitances, but we assume capacitances between stem tissues to be coordinated across species. During field work for the measurements of stem embolism resistance, we sampled short stem segments (~1.5 cm in length; ~1 cm in diameter) for WD measurements. One wood sample was sampled per branch, on the distal extremity of the sample used for the Cavi1000 measurement. The fresh volume of the sample was calculated using an inverse Archimedes principle and a precision balance (CP224S, Sartorius), as the difference between fresh mass and immersed mass of the sample. Dry mass was derived after drying at 103 °C for 3 days. WD was calculated as the ratio between dry mass and fresh volume. In this present study, WD varied from 0.49 to 0.85, whereas WD in the study of Santiago et al. (2018) varied from 0.33 to 0.80.
Leaf and bark minimum conductance
Leaf minimum conductance gmin (mmol m−2 MPa−1; Table 1) was measured between July and November 2017, with the method of weight loss of detached leaves (Blackman et al. 2019b; Duursma et al. 2019). During field work for the measurements of stem embolism resistance, while sampling the branches, strings were tied to sunlit shoots to facilitate later canopy sampling without climbing. gmin was measured on one leaf per tree. Immediately after leaf sampling, leaves were placed in small sealed plastic bags with wet paper towels to avoid dehydration. At the laboratory, the entire leaf surface was gently padded dry with dry paper towels. The cut petiole was sealed with nail polish such that the total leaf transpiration was only mediated by the lamina. Leaves were placed 1 m above air fans and let to dehydrate in a closed air-conditioned room. Air temperature and relative humidity were maintained at ca. 25 °C and ca. 50%, respectively. At regular intervals, leaf mass was recorded with a precision balance (AB 204-S, Mettler Toledo). Time, air temperature, and relative air humidity were noted for each measurement. gmin was calculated as the slope of decreasing leaf mass according to time, in conjunction with VPD—calculated from the known air temperature and relative humidity and divided by the doubled leaf area. Particular attention was paid to the kinetics of water loss, by estimating gmin only during the solely linear phase of leaf water mass decrease with time after stomata had closed.
The bark conductance gbark (mmol m−2 MPa−1; Table 1) was measured during the measurement of leaf embolism resistance, for which a second small branch was sampled. From this branch, three 20-cm-long and ~1-cm-diameter stem segments were sampled, by paying attention to have linear and unbranched stem segments. Then, the segments were placed in small sealed plastic bags with wet paper towels to avoid dehydration and eventual bark shrinkage. At the laboratory, the entire bark surface was dried with paper towels. The two extremities of each stem segment were sealed with melted wax such that the total stem segment transpiration was only mediated by the bark. gbark was measured exactly in the same manner as described for leaves, but the slope of the decreasing water mass of the stem segment over time was divided by the bark surface area. Particular attention was paid to the kinetics of water loss only during the solely linear phase of leaf water mass decrease with time. This also allowed to avoid biases due to the potential release of water that would be just recently absorbed by the bark. The bark surface area was measured by considering the stem segment as a cylinder, based on measurements of stem length and diameter.
Morphological parameters
Shoot leaf area (Aleaf; m2) and shoot bark area (Abark; m2) were quantified during leaf embolism resistance measurements, with a second small branch used for bark conductance measurements only. On this branch, a shoot was sampled, defined as an unbranched stem supporting as many leaves as possible, but with no missing or damaged leaves between the youngest and the oldest leaf. Once sampled from the tree, shoots were placed in sealed plastic bags with wet paper towels to avoid dehydration. At the laboratory, all the surfaces were dried with paper towels. All the leaves were cut and scanned to measure total shoot leaf area (Table 1). The shoot bark area was measured by considering the shoot stem as a cylinder, from length and diameter measurements (Table 1). The stem volume (Vstem; m3) was calculated as a cylinder.
The desiccation time model
To test the effect of vulnerability segmentation on tcrit, we calculated tcrit for species exhibiting a positive vulnerability segmentation (i.e. P88,leaf > P88,stem; Levionnois et al., 2020), representing 12 species. Then, we calculated for the same species a theoretical tcrit with no segmentation, such as P88,leaf = P88,stem. To take into account the vulnerability segmentation in our calculation of tcrit, we used the framework of Blackman et al. (2016) and refined the model. We added two successive desiccation times: (i) leaf desiccation time, from stomatal closure to leaf xylem hydraulic failure, and (ii) stem desiccation time, from leaf xylem to stem xylem hydraulic failure. The model assumes that during phase (i), shoot transpiration is driven by both gmin and gbark; but that during phase (ii), shoot transpiration is driven by gbark only. Contrary to Blackman et al. (2016) we also added the effect of the leaf capacitance after leaf turgor loss point, but before leaf xylem hydraulic failure. We used P88,leaf and P88,stem as parameters for critical leaf and stem hydraulic failure, respectively (Blackman et al. 2016), as P88,stem has been shown to trigger plant mortality for angiosperm species (Urli et al. 2013). Therefore, tcrit_seg for species exhibiting a positive vulnerability segmentation was calculated as:
$$t_{\text{crit\_seg}} = \frac{{\left( {\Psi_{{\text{tlp}}} - P_{{88,{\text{leaf}}}} } \right) * \left( {W_{{ft,{\text{stem}}}} V_{{{\text{stem}}}} + W_{{tlp,{\text{leaf}}}} A_{{{\text{leaf}}}} } \right)}}{{\left( {2A_{{{\text{leaf}}}} g_{\min } + A_{{{\text{bark}}}} g_{{{\text{bark}}}} } \right) * 3600 * VPD}} + \frac{{\left( {P_{{88,{\text{leaf}}}} - P_{{88,{\text{stem}}}} } \right) * W_{{ft,{\text{stem}}}} V_{{{\text{stem}}}} }}{{A_{{{\text{bark}}}} g_{{{\text{bark}}}} * 3600 * VPD}}$$
where Ψtlp is the water potential (MPa) at turgor loss point used as a surrogate of stomatal closure; P88,leaf is the leaf water potential (MPa) at 88% loss of leaf xylem conductivity; P88,stem is the water potential (MPa) at 88% loss of stem xylem conductivity; Wft,stem is the stem capacitance (kg m−3 MPa−1, but divided by the water molar mass of 18.015 × 10−6 kg mmol−1) at full turgor; Wtlp,leaf is the leaf capacitance (mmol m−2 MPa−1) after leaf turgor loss point; Vstem is the stem volume (m3); Aleaf is the shoot leaf area (m2); gmin is the leaf minimum conductance (mmol m−2 s−1); gbark is the bark conductance (mmol m−2 s−1); and VPD is the vapour pressure deficit (mol mol−1). The factor 3,600 converts seconds in hours. Then, for species exhibiting a positive vulnerability segmentation, we artificially cancelled the segmentation by calculating a tcrit_noseg, with P88,leaf = P88,stem, and therefore:
$$t_{\text{crit\_noseg}} = \frac{{\left( {\Psi_{{{\text{tlp}}}} - P_{{88,{\text{stem}}}} } \right) * \left( {W_{{ft,{\text{stem}}}} V_{{{\text{stem}}}} + W_{{{\text{tlp}},{\text{leaf}}}}\, A_{{{\text{leaf}}}} } \right)}}{{\left( {2A_{{{\text{leaf}}}} g_{\min } + A_{{{\text{bark}}}} g_{{{\text{bark}}}} } \right) * 3600 * VPD}}$$
All the parameters of the models and per species are presented in the Table 2. To better characterise how vulnerability segmentation expands tcrit, we calculated additional traits at the shoot and stem levels by combining couples of aforementioned traits (Table 1) that we compared across shoot and stem levels. We calculated leaf minimum transpiration rate (gmin*2Aleaf; mmol s−1) as the product of gmin and shoot leaf area multiplied by 2 (because transpiration occurs at both abaxial and adaxial sides). We calculated bark transpiration rate (gbark*Abark; mmol s−1) at the shoot level. For the Abark considered, we come back to our definition of the leafy shoot, as a single unbranched stem supporting the most leaves, with no missing or damaged leaves between the youngest and the oldest leaf. Then, Abark was directly related to the number of nodes and leaves that constitute the leafy shoot. We calculated shoot capacity to total evaporative surface (Cshoot Aleaf+bark−1; mmol MPa−1 m−2), by multiplying Aleaf by 2. We calculated stem capacity to bark surface (Cstem Abark−1; mmol MPa−1 m−2). Capacity to evaporative surface translates the available stored water which will evaporate during dehydration as a function of total evaporative surface, with a higher capacity to evaporative surface amplifying the positive effect of stored water on drought resistance.
Table 2 List of the tropical rainforest tree species studied with reference to the traits that were used to estimate the desiccation time of shoots Statistical analyses
All statistical analyses were performed in R (R Core Team 2018). Data were tested for normality (Shapiro–Wilk test; α = 0.05). For correlations between traits, we used Pearson or Spearman correlation analyses depending on the normality. Comparison tests were conducted with Student’s, Welch’s, or Mann–Whitney-Wilcoxon’s test, depending on the parameters of the samples (sample size, normality of distribution, variance).
To test for the effect of a given trait on tcrit, it would be appropriate to apply a variance decomposition, which requires a multiple linear model based on the sum of explanatory variables. However, the tcrit model is rather based on products. Switching from a product-based to a sum-based model is feasible with a log transformation. But in this case, this rather leads to a more complex model where the application of variance decomposition would lose its relevance. Therefore, as R2 in bivariate relationships conveys information on explained variance, we calculated R2 for relationships between tcrit (response variable) and a given constitutive trait of the model (predictive variable). This was realised for all traits constitutive of the tcrit model and ordered the relationships according to R2. Then, we assumed that traits with higher R2 have the strongest relative contribution to tcrit.