- © 2010 American Society of Plant Biologists
Abstract
Aquaporins are channel proteins that facilitate the transport of water across plant cell membranes. In this work, we used a combination of pharmacological and reverse genetic approaches to investigate the overall significance of aquaporins for tissue water conductivity in Arabidopsis (Arabidopsis thaliana). We addressed the function in roots and leaves of AtPIP1;2, one of the most abundantly expressed isoforms of the plasma membrane intrinsic protein family. At variance with the water transport phenotype previously described in AtPIP2;2 knockout mutants, disruption of AtPIP1;2 reduced by 20% to 30% the root hydrostatic hydraulic conductivity but did not modify osmotic root water transport. These results document qualitatively distinct functions of different PIP isoforms in root water uptake. The hydraulic conductivity of excised rosettes (Kros) was measured by a novel pressure chamber technique. Exposure of Arabidopsis plants to darkness increased Kros by up to 90%. Mercury and azide, two aquaporin inhibitors with distinct modes of action, were able to induce similar inhibition of Kros by approximately 13% and approximately 25% in rosettes from plants grown in the light or under prolonged (11–18 h) darkness, respectively. Prolonged darkness enhanced the transcript abundance of several PIP genes, including AtPIP1;2. Mutant analysis showed that, under prolonged darkness conditions, AtPIP1;2 can contribute to up to approximately 20% of Kros and to the osmotic water permeability of isolated mesophyll protoplasts. Therefore, AtPIP1;2 can account for a significant portion of aquaporin-mediated leaf water transport. The overall work shows that AtPIP1;2 represents a key component of whole-plant hydraulics.
The plant water status is constantly challenged by diurnal variations in environmental parameters, such as light and temperature, or sustained changes in soil water availability or atmospheric humidity. On the long term, plants respond by adjustments of their hydraulic architecture, mostly through altered root and shoot growth and differentiation. On the short term, plant responses rely on stomatal regulation together with rapid changes in hydraulic conductivities of the root (Lpr) and the leaf (Kleaf).
The hydraulic conductance of living tissues integrates the contribution of parallel paths for water transport, across cell walls (apoplastic path) or from cell-to-cell through plasmodesmata (symplastic path) or membranes (transcellular path). The respective contribution of these paths has been mainly addressed in the context of root water uptake (Steudle and Peterson, 1998). In complement to biophysical analyses, several recent studies have provided strong pharmacological and genetic evidence for an overall role of membranes and water channel proteins (aquaporins) in roots (Maggio and Joly, 1995; Siefritz et al., 2002; Javot et al., 2003; Tournaire-Roux et al., 2003). A comprehensive understanding of how distinct cell layers and individual aquaporin isoforms contribute to the overall water transport capacity of the root and to its dynamic regulation is still being developed (Javot et al., 2003; Bramley et al., 2009). Similar questions have arisen in recent studies addressing the paths that mediate the transport of liquid water in inner leaf tissues, from the veins to the stomatal chamber (Sack and Holbrook, 2006; Heinen et al., 2009).
The overall leaf hydraulic conductance comprises both axial water transport along xylem vessels and transcellular transport in vascular bundles and the mesophyll. In support for a transcellular path, evidence for a role of aquaporins in leaf water transport is emerging. This was first suggested by strong expression of aquaporins in bundle sheath cells (Frangne et al., 2001) or other cell types showing high water permeability (Hachez et al., 2008). In addition, the general aquaporin blocker, mercury, was able to inhibit Kleaf in sunflower (Helianthus annuus) and in six temperate deciduous trees (Aasamaa and Sober, 2005; Nardini et al., 2005). However, the concentrations used were very high (≥ 200 μm HgCl2), and the effects were not reversible. Finally, rapid and reversible changes in Kleaf can be induced by environmental factors such as changes in irradiance (Nardini et al., 2005; Tyree et al., 2005; Sack and Holbrook, 2006) and air and soil humidity (Nardini and Salleo, 2005; Levin et al., 2007). Pressure probe measurements in midrib parenchyma cells of corn leaves revealed that the effects of light (in addition to turgor) on leaf water transport were mediated in part through changes in cell hydraulic conductivity (Kim and Steudle, 2007). The hypothesis that rapid changes in Kleaf involve aquaporin regulation was further substantiated in a study in walnut trees (Cochard et al., 2007). The authors analyzed, using real-time reverse transcription (RT)-PCR, the abundance of two major PIP2 aquaporin transcripts during a transition from dark to high light and found a very good kinetic correlation between the increase in Kleaf and the increase in PIP2 aquaporin expression. Yet, forward or reverse genetic evidence for a role of aquaporins in leaf water transport is lacking.
Because of the limiting role of plasma membranes in transcellular water transport, plasma membrane intrinsic protein (PIP) aquaporins represent the most likely candidates for protein-mediated hydraulic conductivity in roots and leaves (Kaldenhoff et al., 2008; Maurel et al., 2008; Heinen et al., 2009). PIPs occur in two distinct clades. Antisense inhibition of PIP1 and PIP2 expression in transgenic Arabidopsis (Arabidopsis thaliana) and tobacco (Nicotiana tabacum) has indicated a general role for aquaporins of the two classes in root water transport (Kaldenhoff et al., 1998; Martre et al., 2002; Siefritz et al., 2002). More specifically, a specialized role of AtPIP2;2 in osmotic but not hydrostatic root water uptake was uncovered using T-DNA insertion mutagenesis (Javot et al., 2003). Yet, similar dissection has been lacking in the context of leaf water transport. Based on oocyte and yeast expression assays, it was inferred that PIP1 aquaporins may have, with respect to PIP2 aquaporins, a reduced water transport activity (Fetter et al., 2004; Suga and Maeshima, 2004; Sakurai et al., 2008). As a consequence, knowledge on the role of individual PIP1 isoforms in water transport in planta has been lagging.
In this work, we used Arabidopsis to investigate in detail the overall significance of PIP aquaporins to tissue water conductivity. This approach first required the development of novel water transport and pharmacological assays in excised rosettes. These and other assays allowed an accurate reverse genetic analysis of AtPIP1;2 function. This aquaporin (initially referred to as AthH2 or PIP1b) is one of the most abundant PIPs in the root and rosette (Kaldenhoff et al., 1995; Javot et al., 2003; Santoni et al., 2003; Alexandersson et al., 2005; Boursiac et al., 2005).
RESULTS
Isolation of an AtPIP1;2 T-DNA Insertion Mutant
Expression in transgenic Arabidopsis of a chimeric gene comprising 2,248-bp sequence upstream of the AtPIP1;2 coding region fused to a GUS coding sequence induced an intense X-Gluc staining in both roots and shoots (Fig. 1A). In roots, a staining was observed preferentially in the endodermis and stele and to a lesser extent in the cortex (Fig. 1B). A significant expression of PIP1;2:GUS was also observed in all rosette tissues examined, including vascular bundle, bundle sheath, and lamina (epidermis, mesophyll, and stomata; Fig. 1, C and D). These observations roughly confirm a previous GUS expression study employing a somewhat shorter promoter region (Kaldenhoff et al., 1995). They agree with proteomic and transcriptomic analyses indicating that AtPIP1;2 is one of most highly expressed aquaporins in Arabidopsis (Santoni et al., 2003; Alexandersson et al., 2005; Boursiac et al., 2005).
Expression analysis of a PIP1;2-GUS construct. The figure shows the GUS staining of a whole 5-d-old plant grown in vitro (A). GUS staining of a cross section at > 5 mm from a root tip (B; bar =50 μm), of an entire leaf (C), or of a leaf cross section (D; bar = 50 μm) was made in a 21-d-old plant grown in hydroponic conditions.
Two transgenic Arabidopsis lines (SALK_145347 and SALK_19794), each with a T-DNA insertion within the first intron of AtPIP1;2 (Fig. 2A), were obtained from the Nottingham Arabidopsis Stock Centre, and their genomic structure at AtPIP1;2 was confirmed (Fig. 2B). Plants homozygous for either one of the T-DNA insertions, and hereafter referred to as pip1;2-1 and pip1;2-2, were analyzed by RT-PCR. These plants lacked any chimeric AtPIP1;2 transcript encompassing part or the entirety of the T-DNA sequence (data not shown) or any transcript with AtPIP1;2 sequence transcribed downstream of the T-DNA insertion (Fig. 2C). Thus, expression of AtPIP1;2 is fully knocked out in pip1;2-1 and pip1;2-2. We chose pip1;2-1 for complementation by the AtPIP1;2 cDNA, which was placed under the control of a doubled 35S cauliflower mosaic virus promoter and was introduced into pip1;2-1 by Agrobacterium tumefaciens-mediated transformation to yield pip1;2-1Comp lines. RT-PCR analysis showed that expression of AtPIP1;2 transcripts was restored in these lines (Fig. 2C). Wild-type, pip1;2-1, pip1;2-2, and pip1;2-1Comp plants grown in vitro or in soil were morphologically undistinguishable. Root and shoot growth was also characterized in 21-d-old wild-type, pip1;2-1, and pip1;2-1Comp plants grown in hydroponic conditions. The three genotypes showed similar root dry weight (DW) and similar rosette DW and leaf surface (Table I).
Molecular characterization of the pip1;2-1 and pip1;2-2 insertion mutants. A, Physical map of the AtPIP1;2 gene with schematic position of the T-DNA insertions identified in the Salk_145347 and Salk_19794 lines and corresponding to pip1;2-1 and pip1;2-2, respectively (see text). The initiating (ATG) and STOP codons are indicated, with exons shown in black. The numbering of nucleotides refers to the genomic sequence of AtPIP1;2 in BAC clone F4I18. Horizontal arrowheads indicate the positions and orientations of primer sequences used for PCR analysis of the gDNA and resulting cDNA in the genotypes indicated below. B, PCR analysis of gDNA of wild-type (WT), pip1;2-1, and pip1;2-2 plants using a pair of AtPIP1;1-specific primers (1;1f/1;1r) (1), a pair of AtPIP1;2-specific primers (1;2fa/1;2ra) (2), and two primers specific for AtPIP1;2 (1;2ra) and the T-DNA (LBb1), respectively (3). C, RT-PCR analysis of AtPIP1;2 mRNA expression in wild-type, pip1;2-1, pip1;2-2, and pip1;2-1Comp plants. Expression of AtPIP1;2 cDNA was probed with primers (1;2fb/1;2ra) (1) located downstream of the T-DNA insertion site. Amplification of an Elongation Factor1α cDNA fragment was performed for controlling cDNA integrity (2). [See online article for color version of this figure.]
Contribution of AtPIP1;2 to Root Water Transport
The high expression of AtPIP1;2 in roots (Fig. 1; Kaldenhoff et al., 1995; Javot et al., 2003; Santoni et al., 2003; Alexandersson et al., 2005; Boursiac et al., 2005) prompted us to investigate its role in water uptake. The function of AtPIP2;2, another abundantly expressed root aquaporin, was previously unraveled by comparison of osmotic water transport in roots of wild-type and knockout plants (Javot et al., 2003). Using a similar assay, we collected the sap that was spontaneously exuded from roots excised from wild-type and pip1;2-1 plants. Similar sap osmolalities (72–75 mOsmol) and sap flow rates were observed in the two genotypes, which overall indicate similar osmotic hydraulic conductivities (Lpr-o; Table II). To investigate another mode of water transport, we used a pressure chamber device and characterized the hydrostatic pressure dependence of sap flow in roots excised from wild-type, pip1;2-1, and pip1;2-1Comp plants. Corresponding hydrostatic hydraulic conductivity values (Lpr-h) were determined (Javot et al., 2003). With respect to wild-type and pip1;2-1Comp plants, pip1;2-1 showed a statistically significant reduction in Lpr-h by 21% and 31%, respectively, whereas the first two genotypes did not show any statistical difference in Lpr-h (Fig. 3). In another set of experiments, we compared wild-type (n = 10) and pip1;2-2 (n = 14) plants and found that the latter genotype showed a reduction in Lpr-h by 33% ± 4%. The overall data establish a role for AtPIP1;2 in hydrostatic water transport in the Arabidopsis root and a minor if any contribution to osmotic root water transport.
Mean hydrostatic hydraulic conductivity of roots (Lpr-h) from wild-type (WT), pip1;2-1, and pip1;2-1Comp plants. Lpr-h was measured during the daytime in plants grown under a normal photoperiodic regime. Data were pooled from four independent cultures and the indicated number of plants. Values are means ± se, and the asterisk indicates a statistically significant difference (probability < 0.002) from the wild-type value.
Light-Dependent Hydraulic Conductivity of the Arabidopsis Rosette (Kros)
To investigate the water transport properties of Arabidopsis leaf tissues, a novel procedure was developed in which whole excised rosettes that were bathing in a liquid solution were inserted into a pressure chamber. The flow rate of sap (Jv) exuded from the sectioned hypocotyl of an individual plant was proportional to the applied pressure (P) and intercepted the P axis at a balancing pressure close to the origin (P0 = 0.016 ± 0.003 MPa; n = 39; Fig. 4A). Sap exudation was substantially increased (> 2-fold) upon successive section of all leaf blades (Supplemental Fig. S1), suggesting that leaf petioles and blades equally contribute to the hydraulic resistance of the whole rosette. In addition, the Jv(P) relationship was shifted toward higher pressures, with an increase in P0 by approximately 0.1 MPa, when a PEG6000 concentration equivalent to 0.1 MPa was added to the rosette bathing solution. These results suggest that under our experimental conditions, the whole rosette could be assimilated to an osmotic barrier. From the slope of the Jv(P) relationship, a rosette hydraulic conductivity value (Kros ± se) of 149.5 ± 8.7 μL s−1 m−2 MPa−1 (n = 47) was deduced.
Effects of the irradiance regime on rosette hydraulic conductivity (Kros). A, Representative pressure-to-flow relationships measured in rosettes from plants grown under a normal photoperiodic regime and collected around midday (photosynthetically active radiation = 250 μmol photons m−2 s−1; white circles) or plants exposed to a prolonged night (11–21 h darkness; extended darkness; black circles). In both cases, excised rosettes were submerged into a bathing solution, inserted into a pressure chamber, and the flow of sap exuding from the sectioned hypocotyl [Jv(P)] was measured at the indicated pressure as described in “Materials and Methods.” The slope of the regression line is indicative of rosette hydraulic conductance, and together with the cumulated leaf surface allows calculating rosette hydraulic conductivity values (white circles, Kros = 141.2 μL s−1 m−2 MPa−1; black circles, Kros = 223.4 μL s−1 m−2 MPa−1). B, Kros from plants grown under a normal photoperiodic regime (16 h light/8 h dark) and measured around midday (light) or during the night (dark). Kros was also measured in plants exposed to an extended darkness (see text and schematic representation above). Kros was expressed as percentage of the mean control value measured in the light (Kros = 149.5 μL s−1 m−2 MPa−1). The number of individual plants measured in each condition is indicated, and the asterisk indicates a statistically significant difference from control values (probability = 0.009). [See online article for color version of this figure.]
Initial measurements were performed during the day (16-h period at 250 μmol photons m−2 s−1) in rosettes excised > 3 h after the onset of light. Because leaf hydraulic conductance is dependent on irradiance in most of plant species investigated (Tyree et al., 2005; Sack and Holbrook, 2006), we also investigated Kros in rosettes excised during the night. A tendency (probability = 0.07) to an increase in Kros by 38.2% ± 18.2% was observed (Fig. 4B). To possibly observe more marked effects, plants were maintained under darkness by prolonging a normal night by periods of 3 to 10 h. In these conditions, Jv(P) relationships comparable to those recorded in rosettes excised during the day could be recorded (Fig. 4A). Yet, a significant increase (probability = 0.009) in slope was observed, yielding an 88.6% ± 22.4% increase in Kros (Fig. 4B). The dependence of Kros on plant growth conditions supports the idea that this parameter reflects true physiological properties of the Arabidopsis rosette.
Similar to other high-pressure methods, our measurements rely on the principle that under conditions of pressure-induced flow of liquid water the hydraulic resistance of stomatal pores is not limiting with respect to that of internal leaf structures with much smaller conducing diameters (Tyree et al., 2005). Porometer measurements showed that water stomatal conductance (gs ± se; n = 18 plants) of plants at midday or after exposure to extended darkness were 539 ± 33 mmol s−1 m−2 and 90 ± 19 mmol s−1 m−2, respectively. Thus, an increase in Kros was observed in conditions with the lowest gs. These results confirm that, even in conditions of reduced aperture, stomatal pores are not limiting barriers for pressure-dependent liquid flow across the whole rosette.
Effects of Aquaporin Inhibitors on Kros
To test for the contribution of aquaporins to Kros, we first investigated the effects of the common aquaporin blocker, mercury, in conditions where Kros was maximal. Figure 5A shows that in rosettes excised from plants subjected to an extended darkness treatment, exposure to a bathing solution containing 50 μM HgCl2 induced a time-dependent decrease in Jv(P) (Fig. 5A), leading to mean inhibition of Kros by 26.3 ± 4.1% (n = 18; Fig. 6A), with a half-time of t1/2 = 17.8 ± 2.6 min. Azide (NaN3) was previously shown to induce cell acidosis and, therefore, a pH-dependent closure of PIP aquaporins in Arabidopsis roots (Tournaire-Roux et al., 2003). Treatment of the rosette with 2 mm NaN3 induced a decrease in Jv(P), which was very similar in amplitude (23.1% ± 3.7%; n = 17) and time dependency (t1/2 = 27.3 ± 4.3 min) to the mercury-induced effects (Figs. 5B and 6A). Noticeably, this inhibition could be reversed at 82.8% ± 9.6% and with a t1/2 = 21.5 ± 3.4 min upon washout of the inhibitor, indicating that the NaN3 treatment had no irreversible effect on leaf structure or metabolism. By contrast, mercury-induced inhibition of Kros could not be reversed after washout of the inhibitor (1.7% ± 3.0% at 60 min; n = 6).
Time-dependent effects of aquaporin blocking treatments on pressure-induced water transport in rosettes from plants grown under extended darkness. A, Effects of exposure to mercury. An excised rosette was subjected to a constant pressure (P = 0.32 MPa), and Jv(P) was measured over time. The bathing solution was complemented with 50 μm HgCl2 at time t = 0. Fit of the kinetic data by a first-order exponential function indicated a final inhibition of 26.7% with a half-time (t1/2) of 11.4 min. B, Effects of exposure to azide. Same procedure as in A except that 2 mm NaN3, instead of mercury, was added to the bathing solution at t = 0 and was removed after 60 min. The fitted data indicate a maximal inhibition of 19.9%, with a t1/2 = 6.2 min. Reversion occurred with a fitted amplitude of 98.9% and t1/2 of 14.4 min.
Effects of aquaporin blockers on Kros of plants grown under extended darkness (A) or in the light under a normal photoperiodic regime (B). Kros was measured in excised rosettes before (none) and after treatment for 60 min with mercury (50 μm HgCl2) or azide (2 mm NaN3). Data were cumulated from at least four independent cultures, with the indicated number of plants.
In rosettes collected during the day, both 50 μm HgCl2 and 2 mm NaN3 induced an inhibition of Jv(P) with time dependencies similar to those observed in rosettes from dark-grown plants (data not shown). The extent of Kros inhibition was similar with the two treatments (HgCl2, 12.9% ± 1.9%; NaN3, 14.5% ± 1.8%; Fig. 6B) but was significantly lower than in rosettes from plants exposed to extended darkness.
The overall data show that two aquaporin inhibitors, with distinct modes of action, were able to induce similar inhibition of Kros. We also note that the relative effects were the highest in conditions where Kros was the highest (extended darkness, Kros = 261 ± 45.4 μL s−1 m−2 MPa−1; light, Kros = 128.7 ± 8.7 μL s−1 m−2 MPa−1). Thus, the absolute blocking effects of both azide and mercury on Kros were nearly 4 times as high in rosettes from plants subjected to extended darkness than in rosettes from light-grown plants (Fig. 6).
Effects of the Light Regime on PIP Gene Expression
To investigate further the effects of the light regime of leaf aquaporin function, we monitored the expression of all 13 AtPIP genes in leaves of plants grown under light or extended darkness. For this, we used gene-specific primer pairs and quantified the abundance of AtPIP transcripts using real-time RT-PCR analysis in three independent biological experiments (plant cultures). Figure 7 shows the expression ratio of each AtPIP between extended darkness and light. Four genes, including AtPIP1;2 and AtPIP2;6, showed an approximately 2-fold increase in transcript abundance under darkness. AtPIP2;1, which is also highly expressed in leaves (Alexandersson et al., 2005), AtPIP1;4, and AtPIP2;8 were, by contrast, repressed under prolonged darkness. All remaining genes showed a fairly stable expression between the two conditions. The data suggest a complex interplay of PIP isoform function and regulation to determine the hydraulic properties of leaves under various light regimes.
Effects of the light regime on the expression of AtPIP genes in the Arabidopsis rosette. The transcript abundance of each AtPIP gene in whole rosettes was measured by real-time RT-PCR as explained in “Materials and Methods.” The figure shows the mean expression ratio between plants grown under extended darkness and plants grown in the light under a normal photoperiodic regime. Cumulated data (±se) are from three independent biological experiments, each with duplicate PCR reactions. Asterisks indicate significant effects (probability < 0.05) of the light regime.
Contribution of AtPIP1;2 to Kros
The contribution of AtPIP1;2 to Kros was investigated in plants grown under extended darkness because they exhibit the possibly highest activity of leaf aquaporins (Fig. 6) and of AtPIP1;2 in particular (Fig. 7). Pooled data from four independent series of measurements indicated for wild-type and pip1;2-1 plants mean Kros values (μL s−1 m−2 MPa−1 ± se) of 216.7 ± 13.4 (n = 44 plants) and 171.4 ± 6.9 (n = 38 plants), respectively. These results indicate a statistically significant (probability = 0.003) reduction of Kros by 21% in pip1;2-1 with respect to the wild type. Figure 8 shows a representative experiment in which the Kros of pip1;2-1Comp plants was characterized in parallel to that of the two former genotypes. Kros of pip1;2-1Comp was significantly higher than that of pip1;2-1 but similar to the Kros of wild-type plants. The overall data provide evidence that AtPIP1;2 transports water in inner leaf tissues of plants. Because the extent of Kros inhibition in AtPIP1;2 knockout with respect to wild-type plants is in the same range as the extent of Kros inhibition by mercury and azide, the data further suggest that AtPIP1;2 can account for a significant portion of aquaporin-mediated leaf water transport in plants grown under extended darkness.
Kros of wild-type (WT), pip1;2-1, and pip1;2-1Comp plants grown under extended darkness conditions. Kros was measured on the indicated number of plants, as exemplified in Figure 4. Values are means ± se, and the asterisk indicates a statistically significant difference from the wild-type value.
Contribution of AtPIP1;2 to the Water Permeability of Mesophyll Protoplasts
The Kros is determined by the axial conductance of xylem vessels in the petiole and leaf blades and by the conductance of apoplastic and cell-to-cell paths in the vascular bundles and the mesophyll. To estimate the contribution of AtPIP1;2 to cell water transport in the latter tissue, we used a previously described swelling assay in isolated mesophyll protoplasts (Ramahaleo et al., 1999; Martre et al., 2002). More specifically, the protoplast water permeability (Pf) was compared in wild-type, pip1;2-1, and pip1;2-2 plants grown under prolonged darkness. In these conditions, wild-type protoplasts showed broadly distributed Pf values, with a majority of protoplasts with low values (Pf < 8 μm s−1) and a significant subclass with higher values (Fig. 9A). In protoplasts from the two knockout lines, Pf values were less scattered, the subpopulation of protoplasts with high Pf being markedly reduced (Fig. 9A). As a result, mean Pf in these lines was 2-fold lower than in the wild type (Fig. 9B). The data suggest that AtPIP1;2 contributes to water transport in mesophyll cells, this function being the most apparent in the protoplasts with the highest Pf (aquaporin activity).
Pf of mesophyll protoplasts isolated from wild-type (WT), pip1;2-1, and pip1;2-2 plants grown under extended darkness conditions. Cumulated data are from four protoplast preparations from two independent plant cultures (wild type, n = 45; pip1;2-1, n = 32 ; pip1;2-2, n = 35). A, Relative distribution of Pf values in wild-type (black bars), pip1;2-1 (empty bars), and pip1;2-2 (gray bars) protoplasts. B, Mean Pf values (±se).
DISCUSSION
PIP1;2 Contributes to Root Water Transport
Previous studies (Kaldenhoff et al., 1995, 1998; Martre et al., 2002; Siefritz et al., 2002) have addressed the water transporting role of PIP1 homologs using antisense gene expression in transgenic plants. A decrease in leaf protoplast water permeability and, most remarkably, an enhanced growth of roots was observed in transgenic Arabidopsis materials (Kaldenhoff et al., 1998; Martre et al., 2002). The latter phenotype was tentatively interpreted as a compensation for reduced root water permeability to maintain plant water uptake capacity. In support of this, Siefritz et al. (2002) observed a reduced Lpr in tobacco plants expressing the antisense copy of a PIP1 (NtAQP1) cDNA. Aharon et al. (2003) have used another strategy and investigated the function of AtPIP1;2, one of most abundantly expressed PIP1 isoforms in Arabidopsis, by overexpression in tobacco. Transgenic plants showed a spectacular enhancement of growth under favorable conditions but accelerated wilting under drought conditions. It remains unclear, however, whether this phenotype was due to true hydraulic effects of AtPIP1;2 in tobacco tissues, to an indirect stomatal deregulation, or to other unknown effects induced by heterologous expression.
In this work, we used a knockout approach to address the function of AtPIP1;2. Macroarray analysis of aquaporin gene expression (Boursiac et al., 2005) showed that the lack of AtPIP1;2 was not compensated for by changes in expression of any other isoforms (data not shown). Because interactions between PIP isoforms can interfere with their subcellular trafficking (Zelazny et al., 2007), the possibility remains that functional expression of other isoforms at the plasma membrane was altered in PIP1;2 knockout plants. Nevertheless, no alteration in plant growth was observed in the pip1;2-1 mutant both under normal (Table I) and salt stress conditions (data not shown). Yet, disruption of AtPIP1;2 had significant effects (20%–30%) on the root hydrostatic hydraulic conductivity (Lpr-h). By contrast, osmotic water transport (Lpr-o), as assayed by spontaneous exudation of excised roots, was not altered in pip1;2-1. This phenotype differs from that of previously described AtPIP2;2 knockout mutants, which showed a significant alteration in osmotic but not in hydrostatic pressure-dependent water transport (Javot et al., 2003).
Because osmotic gradients within the root determine its exudation capacity, Lpr-o exclusively involves membrane water transport pathways. Pharmacological evidence showed that 80% to 90% of Arabidopsis Lpr-h can also be accounted for by aquaporin activities (Tournaire-Roux et al., 2003), meaning that, even under a purely hydrostatic driving force, the apoplastic path has a modest contribution in this species. Thus, both Lpr-o and Lpr-h result from the integrated water transport capacity of concentric cell layers acting in series. The two parameters were derived, however, from assays differing by the nature and intensity of the local driving forces driving radial water transport. Depending on the assay, the limitation of a cell layer may therefore be purely hydraulic (Lpr-h) or may also depend on its ability to generate a local osmotic driving force (Lpr-o) through solute pumping activity and cell wall tightness. Within this representation, our experimental results suggest a model whereby various root aquaporin isoforms are specialized in distinct modes of water transport, through preferential expression and/or regulation in cell layers with a specialized anatomy and membrane transport protein equipment. It is striking that, although the expression patterns of AtPIP1;2 and AtPIP2;2 in roots are somewhat overlapping, the corresponding knockout phenotypes were so distinct (Javot et al., 2003; this work). This result will certainly stimulate complementary studies, which should combine a thorough analysis of aquaporin expression patterns to cell and whole-root transport assays in a larger number of aquaporin mutant plants and should lead to an integrative modeling of root water transport.
Pressure Chamber Measurements of the Rosette Hydraulic Conductivity (Kros)
Due to the small size of individual Arabidopsis leaves, high-pressure methods commonly used to measure Kleaf cannot be easily applied to this species. In this work, we used whole excised rosettes bathing in a liquid solution and inserted into a pressure chamber. The whole rosette forms a hydraulic network that is definitely more complex than that of a single leaf. Both systems integrate vascular and nonvascular resistances. Here, we show that leaf petioles and blades each contributed to about one-half of the rosette hydraulic resistance (Supplemental Fig. S1). Sack et al. (2002) established the equivalence of Kleaf measurement methods in which trans-leaf water flow was induced by high-pressure, evaporation, or vacuum. The Kros values reported in this work compare properly with the range of Kleaf values measured in Arabidopsis by an evaporative method (Martre et al., 2002) or in other plant species (Sack and Holbrook, 2006). However, other Kleaf values determined in Arabidopsis, also by an evaporative method (Levin et al., 2007), were noticeably lower. One difference was that plants were grown at much lower light (120 μmol photons m−2 s−1) than in the work by Martre et al. (2002) (200 μmol photons m−2 s−1) or in this study (250 μmol photons m−2 s−1). Nevertheless, calculations based on Poiseuille's law have shown that, by comparison to inner leaf tissues, stomata do not exert a significant hydraulic limitation in high-pressure measurements as used in this work (Tyree et al., 2005). In agreement with these theoretical considerations, we were able to detect a 2-fold increase in Kros in conditions where stomatal aperture was reduced by approximately 83%. The significance of our measurements with respect to physiological leaf water transport and aquaporin function was also assessed, as discussed below, by several lines of evidence, including reduction of Kros by aquaporin inhibitors and in aquaporin knockouts or regulation of Kros by light.
Pharmacological and Genetic Evidence for a Role of Aquaporins in Leaf Water Transport
An inhibition of Kleaf by mercury has been reported in sunflower and several tree species and coincided with the highest light-dependent or seasonal Kleaf values (Aasamaa and Sober, 2005; Nardini et al., 2005). However, the significance of this inhibition has remained uncertain because of the high mercury concentrations needed and its lack of reversibility. This work shows consistent effects of two aquaporin inhibitors, at lower concentration and with independent modes of action in two contrasting physiological contexts, that is, under light and extended darkness. The finding that the inhibiting effects of azide were reversible further substantiated our pharmacological approach.
Although reverse genetics can be more straightforward to definitely establish a role of aquaporins in leaf water transport (Martre et al., 2002; Siefritz et al., 2002; Aharon et al., 2003), conclusive studies have been lacking so far. The prerequisite to a knockout approach was to identify the isoforms that are the most highly expressed in leaves. Expression profiling of the aquaporin family has shown that AtPIP1;2, AtPIP2;1, and AtPIP2;6 are among the most highly expressed PIP genes in the Arabidopsis rosette (Alexandersson et al., 2005). Consistent with this, we found that, under extended darkness conditions, AtPIP1;2 can contribute to up to 21% of Kros. As discussed above in the context of the root, the water transport phenotype of AtPIP1;2 knockout rosettes establishes that a genetic dissection of water transport paths and cell hydraulics in leaves has become feasible. We also found that, in accordance to other leaf systems, the Arabidopsis Kros likely integrates a significant axial resistance of vessels, which do not involve aquaporin functions (Sack and Holbrook, 2006). Bundle sheath and mesophyll cells likely represent the other two limiting barriers to liquid water flow (Heinen et al., 2009). We note that AtPIP1;2 was expressed in these two cell types. Whereas water permeability of bundle sheath cells is hardly accessible in Arabidopsis, we tentatively estimated the contribution of AtPIP1;2 to water transport in the mesophyll by measuring the Pf of isolated mesophyll protoplasts. We realize that, in our experimental conditions, most of these cells show a low Pf, suggesting that aquaporins were possibly lowly active in this tissue or down-regulated during protoplast preparation. Nevertheless, the reduced Pf in AtPIP1;2 knockout protoplasts points to a role of AtPIP1;2 in mesophyll water transport. Similar studies, combining expression analysis and phenotypic characterization of knockout mutants for other aquaporin isoforms, will allow us to delineate their respective contributions to water transport in various leaf tissues.
Light-Induced Changes in Kleaf
In this work, we also show that exposure of Arabidopsis plants to darkness increased Kros and its mercury- and azide-sensitive components. Consistent with these effects, a dark treatment enhanced the transcript abundance of several aquaporin genes, including AtPIP1;2. Transcription of certain aquaporin genes has been reported to be under diurnal control (Smith et al., 2004; Bläsing et al., 2005). Because a prolonged darkness induced a further increase in Kros, our data suggest that Kros was not strictly governed by an endogenous circadian mechanism. We also note that the enhancement of PIP transcript abundance was moderate (≤ 2-fold) and that other aquaporin transcripts were down-regulated. Therefore, other mechanisms than transcriptional control may be at work to enhance Kros during darkness.
Diurnal changes in Kleaf have been reported in numerous species, but, in most cases, Kleaf was increased during the day, concomitantly to a higher transpiration demand (Nardini et al., 2005; Tyree et al., 2005; Sack and Holbrook, 2006; Cochard et al., 2007). A midday depression of Kleaf has been reported in a tropical tree species (Simarouba glauca; Brodribb and Holbrook, 2004), but in this case, it was due to a vulnerability of the vascular system to cavitation rather than aquaporin regulation. Therefore, the aquaporin-mediated increase of Arabidopsis Kros at night is somehow atypical. It has been proposed that a high Kleaf, contributed by both xylem vessel conductance and aquaporins, can improve the hydraulic linkage between leaf compartments (for instance, veins and epidermal cells; Ye et al., 2008). As leaf growth can be hydraulically limited (Ehlert et al., 2009; Parent et al., 2009), an aquaporin-mediated increase in Arabidopsis Kros during the night may favor the equilibration of leaf water potentials to prepare the leaf to a metabolically controlled peak of growth right after dawn (Wiese et al., 2007).
Whereas most studies have pointed to dominating effects of light (Sack and Holbrook, 2006; Heinen et al., 2009), the physiological regulations of Kleaf in many species seem to be actually governed by multiple environmental factors. For instance, cell hydraulic conductivity (Lpcell) in midribs of figleaf gourd (Cucurbita ficifolia) cotyledons and maize (Zea mays) leaves (Kim and Steudle, 2007; Lee et al., 2008) was enhanced by both light and high turgor. Overall, leaf water transport was enhanced under low irradiance, i.e. at reduced transpiration, due to a dominating effect of turgor over that of light. By contrast, the two effectors had antagonizing effects under transpiring conditions during the day. In Arabidopsis, the situation seems to be somewhat paradoxical. Studies with plants varying in growth conditions, or exhibiting different abscisic acid concentration or responsiveness, showed that mesophyll protoplast water permeability was strongly correlated to the plant transpiration regime and was maximal at reduced transpiration (Morillon and Chrispeels, 2001). Levin et al. (2007) found by contrast that Kleaf was increased at low relative air humidity that is in conditions where transpiration was the highest. At variance with these results, we observed that Kros was independent from the relative air humidity in which the plants were grown and, in particular, was unchanged at saturating vapor (data not shown). Thus, Kros was truly controlled by irradiance. It is important to note that these different studies where performed on somewhat distinct systems, that is, mesophyll protoplasts (Morillon and Chrispeels, 2001), single leaves (Levin et al., 2007), or excised rosettes (this work).
CONCLUSION
The low or even missing apparent water transport activity of several PIP1 aquaporins after functional heterologous expression has led to the common assumption that PIP1s are poor water channels. Here, we show that AtPIP1;2 significantly contributes to the hydraulic conductivity of both roots and rosette and therefore represents a key component of whole-plant hydraulics. Interestingly, a role in leaf CO2 transport has been proposed for the tobacco homolog NtAQP1 (Flexas et al., 2006; Uehlein et al., 2008). The transport selectivity of AtPIP1;2 and the mechanisms that determine its transport activity and its transcriptional control by multiple factors, including blue light and abscisic acid (Kaldenhoff et al., 1993), will therefore deserve further attention. Importantly, this work, in complement to a previous study (Javot et al., 2003), underscores the power of aquaporin reverse genetics using defined mutants for dissecting the cellular components of plant hydraulics.
MATERIALS AND METHODS
Plant Cultures
All experiments were performed using Arabidopsis (Arabidopsis thaliana) ecotype Columbia. Seeds were surface-sterilized, kept for 2 d at 4°C, and grown in clear polystyrene culture plates at 22°C in the light for 11 d, as described (Javot et al., 2003). Seedlings were then transferred to hydroponic culture. Plants were mounted on a 35 × 35 × 1.8-cm polystyrene raft floating on a basin filled with 8 L of culture medium [1.25 mm KNO3, 0.75 mm MgSO4, 1.5 mm Ca(NO3)2, 0.5 mm KH2PO4, 50 μm FeEDTA, 50 μm H3BO3, 12 μm MnSO4, 0.70 μm CuSO4, 1 μm ZnSO4, 0.24 μm MoO4Na2, and 100 μm Na2SiO3]. Cultures were maintained at a relative humidity of 70% with a 16-h-light (250 μmol photons m−2 s−1) at 22°C/8-h-dark at 21°C cycle, and the culture medium was replaced each week.
For root pressure chamber and root exudation experiments, plants were used 11 to 15 d and 18 to 23 d after transfer in hydroponic conditions, respectively. For leaf water transport assays, plants were used 11 to 15 d after transfer in hydroponic conditions. Plants collected at least 3 h after the onset of the light or night periods were referred to as plants grown in the light or in the dark, respectively. To further investigate the effects of darkness, plants were transferred on the day before measurement, at the end of the photoperiod, into another growth chamber with similar relative humidity and temperature cycle as above, but under complete darkness. Plants were maintained in this chamber for 11 to 21 h before being assayed for leaf water transport. This growth condition was referred to as extended darkness. For real-time RT-PCR experiments, plants were used 12 to 13 d after transfer to hydroponic conditions. Leaves from three to four plants were excised after either a 6-h-light or 14-h-dark period, frozen in liquid nitrogen, and stored at −80°C until RNA extraction.
Molecular Characterization and Complementation of a PIP1;2 T-DNA Insertion Mutant
The Arabidopsis lines SALK_145347 and SALK_19794 were obtained from the Nottingham Arabidopsis Stock Centre (Alonso et al., 2003). The T-DNA insertions in AtPIP1;2 were confirmed by PCR on plant genomic DNA (gDNA) using a combination of primers specific for the T-DNA left border (LBb1: 5′-GCGTGGACCGCTTGCTGCAACT-3 ′) and AtPIP1;2 (1;2ra: 5′-AGTTGCCTGCTTGAGATAAACC-3 ′). The NPTII selectable marker was probably silenced in SALK 145347 as no kanamycin resistance was observed in this line. The line was backcrossed three times with the wild-type parental line and self-pollinated. Two homozygous lines, named pip1;2-1 and pip1;2-2, were identified from SALK_14347 and SALK_19794, respectively, by PCR on gDNA using 1;2ra in combination with a 1;2fa primer (5′-AGTTCACTGGTTTCTCCGAT-3 ′). Integrity of AtPIP1;1 was checked using two gene-specific primers (1;1f, 5′-ACTTCTCCAAGTATACGCCTT-3 ′ ; 1;1r, 5′-CGAAATAATTCTCCTTTGGAAC-3 ′). The absence of functional RNA in pip1;2-1 and pip1;2-2 was checked by RT-PCR using a combination of two AtPIP1;2-specific primers (1;2ra and 1;2fb, 5′-AACCTTTGTCCTTGTTTACACC-3 ′). The cDNA matrix was obtained from RNAs isolated using a Svtotal RNA isolation system (Promega) after reverse transcription with a M-MLV reverse transcriptase (Promega) according to the manufacturer's instructions. Expression of the Elongation Factor1α gene was controlled as described (Javot et al., 2003).
The cauliflower mosaic virus 35S2 expression cassette of a pKYLX 71 vector (Schardl et al., 1987) was excised with EcoRI and ClaI and introduced into a pBSKII+ vector (Stratagene), with its SacI, XbaI, and XhoI sites inactivated. The full-length AtPIP1;2 cDNA was PCR amplified from a pCDM8::PIP1;2 plasmid (Kammerloher et al., 1994) and subcloned into the XhoI site of the modified pBSK vector. The resulting construct was excised using EcoRI and ClaI and subcloned in the corresponding sites of a pGreenII 00179 vector (Hellens et al., 2000). The resulting plasmid was introduced into an Agrobacterium tumefaciens GV3101 strain and used to transform pip1;2-1 by the floral dip method (Clough and Bent, 1998). Hygromycin-resistant plants were self-crossed, and T3 mono-insertional homozygous plants were selected. Transformed plants were screened for expression of AtPIP1;2 by ELISA test using an anti-PIP1 antibody (Santoni et al., 2003) on total protein extracts from 10-d-old in vitro seedlings.
GUS Reporter Construct and Histochemical Analyses
A PIP1;2 promoter fragment encompassing 2,248 bp upstream of the start codon was cloned via GATEWAY recombination into pBGWFS7 (Karimi et al., 2002). The construct results in a translational fusion of five N-terminal amino acids of PIP1;2 with the vector-encoded GFP-GUS fusion protein. Arabidopsis Columbia-0 plants were transformed using floral dip (Clough and Bent, 1998), and independent transgenic lines were selected on soil by herbicide (BASTA) spraying. T2 generation plants were used for histochemical analyses. Staining for GUS enzyme activity was performed in two independent transformed lines on 5-d-old in vitro plantlets or on roots and leaves of 21-d-old plants grown in hydroponic conditions, essentially as described by Javot et al. (2003). Plant materials were transferred into a prefixation buffer (1.5% formaldehyde, 0.05% Triton X-100, and 50 mm phosphate buffer, pH 7.0) for 30 min at room temperature under vacuum and rinsed three times in 50 mm phosphate buffer, pH 7.0. Tissue staining was allowed to proceed by incubation in a revelation buffer (0.5 mm potassium ferricyanure, 0.5 mm potassium ferrocyanure, 1 mm 5-bromo-4-chloro-3-indolyl-GlcUA [Euromedex], and 50 mm phosphate buffer, pH 7.0) at 37°C overnight. Samples were then washed for 5 min at room temperature with 50 mm phosphate buffer, pH 7.0, and at 4°C for 2 h, in a fixation buffer (2% paraformaldehyde, 0.5% glutaraldehyde, and 100 mm phosphate buffer, pH 7.0). Plant and shoot tissues were dehydrated and/or cleared of chlorophyll by incubation in increasing (70%–100%) ethanol concentrations. For additional cross sections, roots and leaves were treated and observed as described (Javot et al., 2003).
DNA Extraction
DNA was extracted by a simplified cetyl-trimethyl-ammonium bromide method essentially as described (Javot et al., 2003). Plant material was ground in liquid nitrogen within a 1.5 mL microcentrifuge tube or alternatively in a bead blender after liquid nitrogen freezing. Each sample was then incubated in 500 μL of extraction buffer (1.4 m NaCl, 20 mm EDTA, 2% [w/v] cetyl-trimethyl-ammonium bromide, 100 mm Tris-HCl, pH 8.0, and 0.4% β -mercaptoethanol added extemporarily). After 30 min at 65°C, each sample was chloroform extracted, and DNA was precipitated twice with isopropanol and finally washed with 70% ethanol, air-dried, and dissolved in 100 μL water. Five microliters of DNA were used for each PCR reaction.
Real-Time RT-PCR
Pairs of primers for gene-specific amplification were designed in the 3′-untranslated transcribed regions of the each of 13 AtPIP cDNAs using primer3 software (http://biotools.umassmed.edu/bioapps/primer3_www.cgi). Their sequences are displayed in Table III. RNA was extracted from leaves of plants grown under light or extended darkness conditions using a SV-RNA isolation kit (Promega) and treated by RQ1 DNAse (1 unit mg−1 RNA) for 1 h at 37°C. cDNAs were obtained as described above and diluted twice before any further reaction. Real-time quantification of leaf RNA was performed using a Light Cycler II (Roche). Individual PCR reaction mixtures contained 1 μL of diluted cDNA, 2 μL of reaction mix (LC Fast startDNA Master Sybr green mix; Roche), and 10 μm forward and reverse primers in 10 μL. Amplification was performed under the following conditions: 15 min at 95°C, followed by 40 cycles with 5 s at 95 ° , 8 s at 62°C, 10 s at 72°C, and temperature transitions of 20°C/s. Finally, a melting curve (consisting of 1 s at 95°C, 30 s at 62°C, and heating at 94°C at a rate of 0.1°C s−1) was determined to ensure amplification specificity. The absence of contaminating gDNA in the cDNA template was checked by running an RT-PCR (45 cycles with an annealing temperature of 52°C) with primers specific for the APT1 gene (At1g27450.1; 5′-CGCCTTCTTCTCGACACTGAG-3 ′ and 5′-CAGGTAGCTTCTTGGGCTTC-3 ′). The two primers allow different size amplifications from cDNA (180 bp) and gDNA (320 bp). Data were analyzed using the Roche Lightcycler software. Cycle threshold (Ct) values were determined by the fit point method from the exponential phase of each amplification. For each gene of interest, PCR efficiency (E) was deduced from a standard dilution series, by the relation E = −1/slope. Relative quantification was determined using the Delta Delta Ct method with E correction and calibration with respect to one experimental condition (light conditions of experiment 2). Overall, a mean Ct value was calculated from three independent biological experiments (plant cultures), each with two PCR replicates. For normalization, four reference genes (TIP41 like, At4g34270; YLS8, At5g08290; GAPC2, At1g13440; and PEX4, At5g25760) were selected on the basis of their expression stability in leaves under light and dark conditions (Czechowski et al., 2005). Using geNORM v3.4 software (Vandesompele et al., 2002), the three more stable genes (YLS8, GAPC2, and PEX4) were selected, and a coefficient of variation was derived for data normalization.
All primers were designed in the 3 ′ untranslated transcribed region. The numbers refer to positions from the initiating ATG codon in the genomic sequences. Primers with an asterisk were similar to those designed by Jang et al. (2004).
Measurements of Root Osmotic Hydraulic Conductivity
Measurements were performed as described by Javot et al. (2003). Briefly, entire root systems of detopped plants were incubated in a culture medium supplemented with 10 mm Glc. After 60 min that allowed spontaneous exudation to reach a steady state level, exuded sap was collected into a graduated glass micropipette, and flow rate (Jv) was measured over the next 60 min. The osmolalities of bath medium (Πs) and sap exuded from individual plants (Πb) were measured by freezing-point depression osmometry. The apparent root osmotic hydraulic conductivity (Lpr-o; in mL g−1 h−1 MPa−1) was deduced from the following equation: Lpr-o = Jv/[mr × (Πb − Πs)], where mr is the overall root dry mass.
Measurement of Root Hydrostatic Hydraulic Conductivity
Measurements were performed essentially as described by Javot et al. (2003) and Boursiac et al. (2005). Briefly, the root system of a freshly detopped plant was inserted into a pressure chamber filled with a PC solution containing 5 mm KNO3, 2 mm MgSO4, 1 mm Ca(NO3)2, and 10 mm MES, pH 6.0, adjusted with KOH. Pressure was then slowly applied to the chamber, and the rate of exuded sap flow (Jv) collected from the sectioned hypocotyl was determined for stabilized hydrostatic pressures (P) between 0.16 and 0.32 MPa. The root DW was determined at the end of the measurement series. The hydrostatic hydraulic conductivity of an individual root system (Lpr-h; in mL g−1 h−1 MPa−1) was calculated from the slope of a plot Jv versus P, divided by the DW of the root system.
Measurement of the Hydrostatic Rosette Hydraulic Conductivity
The entire root system of a hydroponically grown plant was excised by section at the basis of the hypocotyl. The hypocotyl was threaded into a plastic tube, and water tightness was obtained by injection within the tube of low-viscosity dental paste (President Light; Coltene) to embed the hypocotyl upper part and rosette basis. The rosette was then inserted into a pressure chamber filled with a PC solution, the plastic tube being adjusted through the soft plastic washer of the metal lid, and connected to a graduated glass micropipette. Pressure (P) was then slowly applied to the chamber using nitrogen gas. This maneuver resulted in a flow of liquid (Jv) entering through the leaf surface and exiting from the hypocotyl section. In preliminary measurements performed on about 40 rosettes, the Jv(P) relationship determined for 0.1 < P < 0.7 MPa indicated a linear relationship with an intercept of the x axis at approximately 0 MPa. The pressure tightness of the rosette-hypocotyl continuum after insertion in the pressure chamber device was established by showing that addition in the bathing solution of 0.078 g PEG6000/g water, corresponding to a 0.1 MPa osmotic pressure, resulted in similar shift of the Jv(P) curve toward higher P. In routine measurements, Jv was determined over successive 10- to 20-min periods for at least three stabilized P values between 0.16 and 0.32 MPa. At the end of the measurement series, the rosette was removed, leaves were excised and scanned, and their surface area was measured using image analysis software (Optimas-Bioscan V.6-1) to determine the overall rosette surface area (Sros). The hydraulic hydrostatic conductivity of an individual rosette (Kros; μL s−1 m−2 MPa−1) was calculated from the following equation: Kros = Jv/[Sros × P].
Effects of aquaporin inhibitors were determined at a constant pressure of 0.32 MPa by monitoring the time-dependent changes of Jv following addition of the inhibitor into the rosette bathing solution.
Protoplast Preparation and Measurement of Water Permeability (Pf)
Mesophyll protoplasts were prepared as described (Ramahaleo et al., 1999; Martre et al., 2002) by incubating leaf tissues in solution A (0.57 m sorbitol, 0.5 mm CaCl2, 0.5 mm MgCl2, 0.5 mm ascorbic acid, and 5 mm MES, pH 5.5) complemented with 1.5% cellulase RS and 0.25% pectolyase Y23. Isolated protoplasts were resuspended in solution A, and swelling measurements were performed at 20°C by transfer of individual protoplasts into a hypotonic solution (solution A but with 0.37 m sorbitol instead of 0.57 m sorbitol) using the procedures described by Ramahaleo et al. (1999).
Supplemental Data
The following materials are available in the online version of this article.
Supplemental Figure S1. Hydrostatic hydraulic conductivity of whole rosettes or of rosettes with all leaf blades excised.
Acknowledgments
We are grateful to Gaëlle Viennois for help in GUS histochemical analyses, to Lionel Verdoucq for discussions, and to Birgit Geist for excellent technical assistance.
Footnotes
↵1 This work was supported in part by a grant from the French Ministry of Research (ACI2003 “Biologie du Développement et Physiologie Intégrative”), by the Agence Nationale de la Recherche (ANR–05–GPLA–034–06 and ANR–07–BLAN–0226), and by the Deutsche Forschungsgemeinschaft (SPP1108, Scha 454/8).
↵2 These authors contributed equally to the article.
↵3 Present address: UMR INRA/USTL, Estrées-Mons BP 50136, F–80203 Peronne, France.
The author responsible for distribution of materials integral to the findings presented in this article in accordance with the policy described in the Instructions for Authors (www.plantphysiol.org) is: Christophe Maurel (maurel{at}supagro.inra.fr).
↵[C] Some figures in this article are displayed in color online but in black and white in the print edition.
↵[W] The online version of this article contains Web-only data.
- Received July 24, 2009.
- Accepted December 21, 2009.
- Published December 24, 2009.