Water transport in barley roots

Radial transport of water in excised barley (Hordeum distichon, cv. Villa) roots was measured using a new method based on the pressure-probe technique. After attaching excised roots to the probe, root pressures of 0.9 to 2.9 bar were developed. They could be altered either by changing the root pressure artificially (with the aid of the probe) or by changing the osmotic pressure of the medium in order to induce water flows across the root. The hydraulic conductivity of the barley roots (per cm² of outer root surface) was obtained in different types of experiments (initial water flow, pressure relaxations, constant water flow) and was (0.3–4.3)·10^-7 cm s^-1 bar^-1. The hydraulic conductivity of the root was by an order of magnitude smaller than the hydraulic conductivity of the cell membranes of cortical and epidermal cells (0.8–2.2)·10^-6 cm s^-1 bar^-1. The half-times of water exchange of these cells was 1–21 s and two orders of magnitude smaller than that of entire excised roots (100–770 s). Their volumetric elastic modulus was 15–305 bar and increased with increasing turgor. Within the root cortex, turgor was independent of the position of the cell within a certain layer and turgor ranged between 3 and 5 bar. The large difference between the hydraulic conductivity of the root and that of the cell membranes indicates that there is substantial cell-to-cell (transcellular plus symplasmic) transport of water in the root. When it is assumed that 10–12 membrane layers (plasmalemma plus tonoplast) in the epidermis, cortex and endodermis form the hydraulic resistance to water flow, a value for the hydraulic conductivity of the root can be calculated which is similar to the measured value. This picture for water transport in the root contradicts current models which favour apoplasmic water transport in the cortex.     

Characteristics of Hg- and Zn-sensitive Water Channels in the Plasma Membrane of Chara Cells*

Hydraulic conductivity (L_p) of the plasma membrane of Chara corallina was inhibited by HgCl₂ maximally by about 95%. The inhibition was reversed by 2-mercaptoethanol, reconfirming the observation obtained by Henzler and Steudle (1995). The results suggest that osmotic water transport through Chara cells occurs mostly via mercury-sensitive water channels containing thiol groups. ZnCl₂ dissolved in APW (pH 5.6) also inhibited L_p by about 80% within 1–2 h, while ZnCl₂ dissolved in Hepes-Tris buffer (pH 7.4) inhibited it by about 90% within several minutes. Inhibition of L_p by ZnCl₂ was also reversed by 2-mercaptoethanol, suggesting that zinc acts also on thiol groups of water channel proteins. Cells from which tonoplast had been removed by ECTA were as sensitive to both HgCl₂ and ZnCl₂ (pH 7.4) as normal cells. This demonstrates that water channels sensitive to thiol reagents really exist in the plasma membrane. On the other hand, ZnCl₂ (pH 5.6) did not inhibit L_p of tonoplast-free cells. This may be accounted for by assuming first that Hg- and Zn-sensitive thiol groups of water channels may exist on the cytoplasmic side, and second that ZnCl₂ in acidic medium may exist in ionized species which can be chelated by EGTA after permeation. The polar water permeability, or the endoosmotic L_p being larger than the exoosmotic one, was not affected by lowering the rate of osmosis by decreasing the osmotic gradient for transcellular osmosis down to 0.02 M sorbitol. The polarity disappeared when osmotic water flow through water channels was completely inhibited by HgCl₂. Thus the polarity is assumed to be intrinsic to water channels in the plasma membrane.     

The integration of whole-root and cellular hydraulic conductivities in cereal roots

The hydraulic conductivities of excised whole root systems of wheat (Triticum aestivum L. cv. Atou) and of single excised roots of wheat and maize (Zea mays L. cv. Passat) were measured using an osmotically induced back-flow technique. Ninety minutes after excision the values for single excised roots ranged from 1.6·10^-8 to 5.5·10^-8 m·s^-1·MPa^-1 in wheat and from 0.9·10^-8 to 4.8·10^-8 m·s^-1·MPa^-1 in maize. The main source of variation was a decrease in the value as root length increased. The hydraulic conductivities of whole root systems, but not of single excised roots, were smaller 15 h after excision. This was not caused by occlusion of the xylem at the cut end of the coleoptile. The hydraulic conductivities of epidermal, cortical and endodermal cells were measured using a pressure probe. Epidermal and cortical cells of both wheat and maize roots gave mean values of 1.2·10^-7 m·s^-1·MPa^-1 but in endodermal cells (measured only in wheat) the mean value was 0.5·10^-7 m·s^-1·MPa^-1. The cellular hydraulic conductivities were used to calculate the root hydraulic conductivities expected if water flow across the root was via transcellular (vacuole-to-vacuole), apoplasmic or symplasmic pathways. The results indicate that, in freshly excised roots, the bulk of water flow is unlikely to be via the transcellular pathway. This is in contrast to our previous conclusion (H. Jones, A.D. Tomos, R.A. Leigh and R.G. Wyn Jones 1983, Planta 158, 230–236) which was based on results obtained with whole root systems of wheat measured 14–15 h after excision and which probably gave artefactually low values for root hydraulic conductivity. It is now concluded that, near the root tip, water flow could be through a symplasmic pathway in which the only substantial resistances to water flow are provided by the outer epidermal and the inner endodermal plasma membranes. Further from the tip, the measured hydraulic conductivities of the roots are consistent with flow either through the symplasmic or apoplasmic pathways.Symbols L _{p, cell} cell hydraulic conductivity - L _{p, root} root hydraulic conductivity - L _{p, root} calculated root hydraulic conductivity - root reflection coefficient     

Turgor pressure changes trigger characteristic changes in the electrical conductance of the tonoplast and the plasmalemma of the marine alga Valonia utricularis

The giant marine alga Valonia utricularis is capable of regulating its turgor pressure in response to changes in the osmotic pressure of the sea water. The turgor pressure response comprises two phases, a fast, exponential phase arising exclusively from water shifting between the vacuole and the external medium (time constant about 10 min) and a second very slow, almost exponential phase adjusting (but not always) the turgor pressure near to the original value by release or uptake of KCl (time constant about 5 h). The changes in the vacuolar membrane potential as well as in the individual conductances of the tonoplast and plasmalemma accompanying turgor pressure regulation were measured by using the vacuolar perfusion assembly (with integrated microelectrodes, pressure transducers and pressure‐regulating valves) as described by Wang et al. (J. Membrane Biology 157, 311–321, 1997). Measurements on pressure‐clamped cells gave strong evidence that the turgor pressure, but not effects related to water flow (i.e. electro‐osmosis or streaming potential) or changes in the internal osmotic pressure and in the osmotic gradients, triggers the cascade of osmotic and electrical events recorded after disturbance of the osmotic equilibrium. The findings definitely exclude the existence of osmosensors as postulated for other plant cells and bacteria. There was also evidence that turgor pressure signals were primarily sensed by ion transporters in the vacuolar membrane because conductance changes were first recorded in the many‐folded tonoplast and then significantly delayed in the plasmalemma independent of the direction of the osmotic challenge. Consistently, turgor pressure up‐regulation (but not down‐regulation) could be inhibited reversibly by external addition of the K⁺ transport inhibitor Ba²⁺ and/or by the Cl^– transport inhibitor 4,4′‐diisothiocyanatostilbene‐2,2′‐disulfonic acid (DIDS). Extensive studies under iso‐, hyper‐ and hypo‐osmotic conditions revealed that K⁺ and Cl^– contribute predominantly to the plasmalemma conductance. Addition of 0.3 mm NaCN showed further that part of the K⁺ and Cl^– transporters depended on ATP. These transporters are apparently up‐regulated upon hyper‐osmotic, but not hypo‐osmotic challenge. These findings explain the strong increase of the K⁺ influx upon lowering turgor pressure and the less pronounced pressure‐dependence of the Cl^– influx of V. utricularis reported in the literature. The data derived from the blockage experiments under hypo‐osmotic conditions were also equally consistent with the experimental findings that the K⁺ efflux is solely passive and progressively increases with increasing turgor pressure due to an increase of the volumetric elastic modulus of the cell wall. However, despite unravelling some of the sequences and other components involved in turgor pressure regulation of V. utricularis the co‐ordination between the ion transporters in the tonoplast and plasmalemma remains unresolved because of the failure to block the tonoplast transporters by addition of Ba²⁺ and DIDS from the vacuolar side.     

Compartment analysis of plant cells by means of turgor pressure relaxation: I. Theoretical considerations

Summary Turgor pressure relaxation curves for individual plant cells represent an important source of information for the plant physiologist. However, the accurate interpretation of these curves is strongly dependent on the model chosen to describe the plant cell. If the compartmentation of the cell into vacuole and cytoplasm is taken into account, a theoretical analysis shows that pressure relaxation curves can be represented by the sum of two exponential functions. Givena priori assumptions about the exchange area of the tonoplast and its reflection coefficient, the hydraulic conductivities of the plasmalemma and tonoplast can be determined and the proportion of the total cell volume occupied by the cytoplasm is also obtained. Numerical solutions to the flow equations have shown that the biphasic nature of pressure relaxations is maintained even when a permeable tonoplast is assumed. Depending on the magnitude of the reflection coefficient and the permeability of the vacuolar membrane, large errors can arise in the determination of the hydraulic conductivity of the tonoplast. However, under certain conditions, even a highly permeable tonoplast may behave like a nonpermeable membrane during pressure relaxation.     

Participation of Ca2+ in cessation of cytoplasmic streaming induced by membrane excitation inCharaceae internodal cells

Summary The mechanism of the cessation of cytoplasmic streaming upon membrane excitation inCharaceae internodal cells was investigated.Cell fragments containing only cytoplasm were prepared by collecting the endoplasm at one cell end by centrifugation. In such cell fragments lacking the tonoplast, an action potential induced streaming cessation, indicating that an action potential at the plasmalemma alone is enough to stop the streaming.The active rotation of chloroplasts passively flowing together with the endoplasm also stopped simultaneously with the streaming cessation upon excitation. The time lag or interval between the rotation cessation and the electrical stimulation for inducing the action potential increased with the distance of the chloroplasts from the cortex. The time lag was about 1 second/15 m, suggesting that an agent causing the rotation cessation is diffused throughout the endoplasm.Using internodes whose tonoplast was removed by replacing the cell sap with EGTA-containing solution (tonoplast-free cells,Tazawa et al. 1976), we investigated the streaming rate with respect to the internal Ca²⁺ concentration. The rate was roughly identical to that of normal cells at a Ca²⁺ concentration of less than 10^–7 M. It decreased with an increase in the internal Ca²⁺ concentration and was zero at 1 mM Ca²⁺.The above results, together with the two facts that Ca²⁺ reversibly inhibits chloroplast rotation (Hayama andTazawa, unpublished) and the streaming in tonoplast-free cells does not stop upon excitation (Tazawa et al. 1976), lead us to conclude that a transient increase in the Ca²⁺ concentration in the cytoplasm directly stops the cytoplasmic streaming. Both Ca influxes across the resting and active membranes were roughly proportional to the external Ca²⁺ concentration, which did not affect the rate of streaming recovery. Based on these results, several possibilities for the increase in Ca²⁺ concentration in the cytoplasm causing streaming cessation were discussed.     

Water-relation parameters of epidermal and cortical cells in the primary root ofTriticum aestivum L.

Water-relation parameters of root hair cells, hairless epidermal cells, and cortical cells in the primary root of wheat have been measured using the pressure-probe technique. Under well-watered conditions the mean cell turgor of cortical cells was 6.8±1.9 (30) bar (mean±SD; the number of observations in brackets). In hairless epidermal and root hair cells the mean cell turgor was 5.5±1.9 (22) and 4.4±1.5 (15) bar, respectively. Despite the large variability, turgor pressure was significantly lower (confidence interval=0.95) in epidermal cells relative to cortical cells. This may be a consequence of the ultrafiltration of ions by the external cell wall and-or plasmalemma of epidermal cells. The volumetric elastic modulus of the cells ranged from 10 to 150 bar. This parameter was dependent on cell volume, but within experimental accuracy, was independent of cell type. No pressure dependence of the volumetric elastic modulus was observed in these cells. The half-times for water exchange ranged from 1.8 to 48.8 s. The mean value increased in the order root hair < hairless epidermal < cortical cells and was directly related to volume to surface area ratio. Thus the hydraulic conductivities of the three cell types were similar and averaged 1.2±0.9·10^-6 (170) cm s^-1 bar^-1. No polarity was observed between inwardly and outwardly directed water flow. The similarity of the hydraulic conductivities of root hairs to those of other cells indicates that the membranes of root hairs are not particularly specialized for water transport. The overall hydraulic conductivity for radial water flow across the root was estimated from the pressure-probe data using a simple model and was compared with that measured directly on whole roots using an osmotic backflow technique. It was tentatively concluded that upon sudden osmotic perturbation, the major pathway for water transfer across the root may be through the symplasm and involve net flow from vacuole to vacuole.     

Intracellular perfusion and cell centrifugation studies on plasmalemma transport processes inChara corallina

Summary The OH^– transport system ofChara corallina was studied using the techniques of intracellular perfusion and cell centrifugation. Application of silk ligatures to internodal cells had quite a perturbative effect on the OH^– transport activity. Approximately 12 hr were required before normal pH profiles were reestablished.Tonoplast-free internodal cells developed rather weak, uniform alkalinity along the cell surface. Redevelopment of control pH patterns was never observed in these experiments. Surface pH profiles similar to those observed on tonoplast-free cells could also be obtained by subjecting cells to mild centrifugation (180×g). Organelles of the streaming cytoplasm were contained within the centrifugal cell segment by applying a ligature near the cell center. Normal pH profiles were observed along the centrifugal segment, while the centripetal segment developed weak, rather uniform alkaline profiles. Upon redistribution of the cytoplasmic organelles, normal pH profiles were established along the entire cell length.These results indicate that an organelle within the streaming cytoplasmic phase is responsible for the spatial location and control over OH^– transport. This explains the absence of control pH profiles in tonoplast-free cells, since during the disintegration of the tonoplast, most of the streaming cytoplasm coagulates at one end of the cell.Parallel pH mapping and electrophysiological studies indicated that the plasmalemma of this species contains an ATP-dependent electrogenic H⁺ transport system. Also, experiments conducted in the presence and absence of cellular ATP demonstrated that OH^– efflux can be driven passively by the membrane potential. Whether OH^– transport is strictly a passive process in normal cells remains to be resolved.     

Aquaporins and cell growth

This review covers the data concerning the relationship between cell growth and aquaporins in the cell membranes, the plasmalemma and tonoplast. Genes of aquaporins, water channel-forming proteins, are actively expressed before the onset and during cell elongation, thus providing accumulation of aquaporin protein and higher membrane hydraulic conductivity. As a result, an additional water uptake favors cell vacuolation and elongation. The review gives information on all growing plant organs. In actively dividing plant cells, only plasmalemma aquaporins are synthesized, whereas in elongating cells, tonoplast aquaporins are synthesized as well. The review includes also the findings of aquaporin research after growth completion.     

Membrane depolarization induced by transcellular osmosis in internodal cells ofNitella flexilis

Summary Membrane depolarization induced by transcellular osmosis was studied using internodal cells ofNitella flexilis. Transcellular osmosis was induced by using sorbitol or methanol as the osmotic agent. In the endosmotic cell half, the membrane often generated an action potential and depolarized further with a concomitant decrease in membrane resistance. This osmosis-induced depolarization was a graded response dependent on the external osmotic gradients. However, in the exosmotic cell half, both membrane potential and membrane resistance changed insignificantly. Membrane depolarization occurred also in cells made inexcitable by bathing in 0.1–1 mM KCl solution.Effects of temperature and internal osmotic pressure on osmosis-induced depolarization were investigated. The magnitude of depolarization at low temperature (2 or 4°C) was larger than that at room temperature (around 20°C). Membrane depolarization was accelerated by lowering the internal osmotic pressure and inhibited by raising it.Not only the plasmalemma but the tonoplast also responded significantly to endosmosis.     

Nature of the water channels in the internodal cells ofNitellopsis

Summary The hydraulic resistance was measured on internodal cells ofNitellopsis obtusa using the method of transcellular osmosis. The hydraulic resistance was approximately 2.65 pm^–1 sec Pa, which corresponds to an osmotic permeability of 101.75 m sec^–1 (at 20°C).p-Chloromercuriphenyl sulfonic acid (pCMPS) (0.1–1mm, 60 min) reversibly increases the hydraulic resistance in a concentration-dependent manner.pCMPS does not have any effect on the cellular osmotic pressure.pCMPS increases the activation energy of water movement from 16.84 to 32.64 kJ mol^–1, indicating that it inhibits water movement by modifying a low resistance pathway.pCMPS specifically increases the hydraulic resistance to exosmosis, but does not influence endosmosis. By contrast, nonyltriethylammonium (C₉), a blocking agent of K⁺ channels, increases the hydraulic resistance to endosmosis, but does not affect that to exosmosis. These data support the hypothesis that water moves through membrane proteins in characean internodal cells and further that the polarity of water movement may be a consequence of the differential gating of membrane proteins on the endo- and exoosmotic ends.     

Osmotic Water Permeability of Vacuolar and Plasma Membranes Isolated from Maize Roots

The method of stopped flow was used to follow the changes in light scattering by the vesicles of plasmalemma and tonoplast isolated from maize (Zea maysL.) roots and treated by osmotic pressure. In both membrane preparations, the rate of the process depended on the osmotic gradient and was described with the simple exponential function. The rate constants derived from these functions were the following: the coefficient of water permeability in the tonoplast (P= 165 ± 7 m/s) exceeded by an order of magnitude the corresponding index for plasmalemma (11 ± 2 m/s). The presence of HgCl₂(1.6 nmol/g membrane protein) decreased the tonoplast water permeability by 80%. Microviscosity studies of the hydrocarbon zone in the isolated membranes by using a fluorescent diphenylhexatriene probe demonstrated that the two membranes do not differ in the phase state of their lipid bilayer. The authors conclude that the observed difference in water permeability does not depend on the state of the lipid phase and probably reflects the dissimilar functional activity of plasmalemma and tonoplast aquaporins.     

Separate Determination of the Electrical Properties of the Tonoplast and the Plasmalemma of the Giant-Celled Alga Valonia utricularis: Vacuolar Perfusion of Turgescent Cells with Nystatin and Other Agents

In the giant-celled marine algae Valonia utricularis the turgor-sensing mechanism of the plasmalemma and the role of the tonoplast in turgor regulation is unknown because of the lack of solid data about the individual electrical properties of the plasmalemma and the vacuolar membrane. For this reason, a vacuolar perfusion technique was developed that allowed controlled manipulation of the vacuolar sap under turgescent conditions (up to about 0.3 MPa). Charge-pulse relaxation studies on vacuolarly perfused cells at different turgor pressure values showed that the area-specific resistance of the total membrane barrier (tonoplast and plasmalemma) exhibited a similar dependence on turgor pressure as reported in the literature for nonperfused cells: the resistance assumed a minimum value at the physiological turgor pressure of about 0.1 MPa. The agreement of the data suggested that the perfusion process did not alter the transport properties of the membrane barrier. Addition of 16 μm of the H⁺-carrier FCCP (carbonylcyanide p-trifluoromethoxyphenyhydrazone) to the perfusion solution resulted in a drop of the total membrane potential from +4 mV to −22 mV and in an increase of the area-specific membrane resistance from 6.8 × 10⁻² to 40.6 × 10⁻²Ωm². The time constants of the two exponentials of the charge pulse relaxation spectrum increased significantly. These results are inconsistent with the assumption of a high-conductance state of the tonoplast (R. Lainson and C.P. Field, J. Membrane Biol. 29:81–94, 1976). Depending on the site of addition, the pore-forming antibiotics nystatin and amphotericin B affected either the time constant of the fast or of the slow relaxation (provided that the composition of the perfusion solution and the artificial sea water were replaced by a cytoplasma-analogous medium). When 50 μm of the antibiotics were added externally, the fast relaxation process disappeared. Contrastingly, the slow relaxation process disappeared upon vacuolar addition. The antibiotics cannot penetrate biomembranes rapidly, and therefore, the findings suggested that the fast and slow relaxations originated exclusively from the electrical properties of the plasmalemma and the tonoplast respectively. This interpretation implies that the area-specific resistance of the tonoplast is significantly larger than that of the plasmalemma (consistent with the FCCP data) and that the area-specific capacitance of the tonoplast is unusually high (6.21 × 10⁻² Fm⁻² compared to 0.77 × 10⁻² Fm⁻² of the plasmalemma). Thus, we have to assume that the vacuolar membrane of V. utricularis is highly folded (by a factor of about 9 in relation to the geometric area) and/or contains a fairly high concentration of mobile charges of an unknown electrogenic ion carrier system. Received: 22 October 1996/Revised: 16 January 1997     

A New Turgor/Membrane Potential Probe Simultaneously Measures Turgor and Electrical Membrane Potential

Abstract: A new combined turgor/membrane potential probe (T-EP probe) monitored cell turgor and membrane potential simultaneously in single giant cells. The new probe consisted of a silicone oil-filled micropipette (oil-microelectrode), which conducted electric current. Measurements of turgor and hydraulic conductivity were performed as with the conventional cell pressure probe besides the membrane potential. In internodal cells of Chara corallina, steady state turgor (0.5-0.7 MPa) and resting potentials (-200 to ?220 mV) in APW, and hydraulic conductivity (0.07 to 0.21 × 10～⁵ m s^?1 MPa^?1) were measured with the new probe, and cells exhibited healthy cytoplasmic streaming for at least 24 h during measurements. When internodal cells of Chara corallina were treated with 30, 20, 10, and 5 mM KCI, turgor responded immediately to all concentrations, and the osmotic changes in the medium were measured. Action potentials, which brought the membrane potential to a steady depolarization that measured the concentration difference of K⁺ in the medium, were induced in a concentration — dependent delay and occurred only 30, 20, and 10 mM of KCl. When the solution was changed back to APW, the repolarization of membrane potential consisted of a quick and a following slow phase. During the quick phase, which took place immediately and lasted 1 to 3 min, the plasma membrane remained activated. The membrane was gradually deactivated in the slow phase, and entirely deactivated when the membrane potential recovered to the resting potential in APW. Although the activated plasma membrane was permeable to K⁺, no major ion channels were activated on the tonoplast, and therefore, internodal cells of Chara corallina did not regulate turgor when osmotic potential changed in the surrounding medium.     

The proton pumps of the plasmalemma and the tonoplast of higher plants

Studies on intact cells, membrane vesicles, and reconstituted proteoliposomes have demonstrated in higher plants the existence of an ATP-driven electrogenic proton pump operating at the plasmalemma. There is also evidence of a second ATP-driven H⁺ pump localized at the tonoplast. The characteristics of both these ATP-driven pumps closely correspond to those of the plasmalemma and tonoplast proton pumps ofNeurospora and yeasts.     

Reversible inhibition of cytoplasmic streaming by intracellular Ca2+ in tonoplast-free cells ofChara australis

Summary The effect of the intracellular concentration of Ca²⁺ on the cytoplasmic streaming of tonoplast-free cells ofChara australis was studied by intracellular perfusion. The perfusion media contained 1 mM Mg · ATP. Both cell ends were cut and left open. Media of different Ca²⁺ concentrations were perfused through the cell and the rate of the cytoplasmic streaming just after perfusion was measured. The critical concentration of Ca²⁺ for inhibiting the streaming was 5 × 10^–4M, which was substantially higher than that found earlier byWilliamson (1975) andHayama et al. (1979). Recovery from the inhibition occurred, though not completely, by removing Ca²⁺.In tonoplast-free cells the Ca²⁺ sensitivity differed according to the culture conditions. Cells cultured indoors exhibited a higher sensitivity than those cultured outdoors. Theformer cells contained granule-rich endoplasm aggregates after loss of the tonoplast, while the latter cells did no such aggregates. The aggregates were fixed to the cortical gel with a high dosage of Ca²⁺ and freed by removing it.     

The site of penetration resistance to water in plant protoplasts

Summary The main purpose of this investigation was to determine the primary site of resistance to the penetration of water in the protoplasm of inner epidermal cells of theAllium cepa bulb scale. Since it is known that the tonoplast has a very high water permeability, it was left to decide whether the mesoplasm and/or the plasmalemma is the main barrier. According to a theory ofHöfler, the mesoplasm is the main barrier. Because it is not possible to isolate the plasmalemma, the influence of the mesoplasm was removed by causing rosette systrophy. In rosette systrophy, almost all of the mesoplasm is collected arround the nucleus and the tonoplast and plasmalemma lie adjacent in the greater part of the protoplast.Cells with and without systrophy are found in the same preparation but show no great difference in water permeability. The systrophied cells have even a lower water permeability constant than the non-systrophied cells. This indicates clearly that the mesoplasm is of no significant importance for water permeability, and that the primary site of penetration resistance to water is the plasmalemma.It was possible to measure the water permeability constants of tonoplasts. While the 2 K_wo values for protoplasts are approximately 6–8×10^–4 cm/sec, those for tonoplasts are about 100 times higher.The water permeability constants found with glucose solutions were essentially the same as those found in solutions of KCl + CaCl₂. Other less inert substances, such as EDTA, give different (higher) values.Using the method of partial deplasmolysis and plasmolysis, it was possible to change the protoplast volume several times, once until the eight time in K-Ca solutions and until the fifth time in glucose solutions.The water permeability constants do not change appreciably, neither in the sequential plasmolysis steps nor between deplasmolysis and plasmolysis. Yet there is a small but significant difference between deplasmolysis and plasmolysis values. The deplasmolysis values are slightly higher.In the K-Ca solutions the tonoplasts which were formed showed a linear expansion which indicates ion permeability. Permeability constants are 0.003–0.006×10^–4 cm/sec, about in the same range as those of moderate anelectrolyte permeability.     

Membrane alterations in winter rye and Brassica napus cells during lethal freezing and plasmolysis

Abstract Cells fixed during freezing or plasmolysis were used to study membrane alterations in hardened and non-hardened Brassica napus suspension-cultured cells and rye leaf mesophyll cells. The plasmalemma in non-hardened rye mesophyll cells formed multilamellar vesicles during lethal freezing at high subzero temperatures (–5°C). These vesicles became highly condensed at lower subzero temperatures (–10°C). Conversely, cold-hardened rye mesophyll cells did not undergo membrane alterations at these temperatures. The results from plasmolysis of B. napus and rye mesophyll cells hardened by ABA at 25 °C and low temperature (2°C), respectively, verify the cell response to lethal freezing. Again there was a continuum of responses with 1 kmol m^?3 balanced salt causing multilamellar protrusions. Appression of the plasmalemma against the tonoplast to form multilamellar vesicles and the invagination of these vesicles into the tonoplast were also observed in rye cells undergoing lethal plasmolysis. Increasing the plasmolysing solution to 3 kmol m^?3 occasionally caused the formation of multilamellar vesicles on the cell surface of hardened rye mesophyll cells.     

Determination of the hydraulic conductivity and of reflection coefficients in Nitella flexilis by means of direct cell-turgor pressure measurements

From direct and continuous measurements of the internal hydrostatic pressure (P) in the internodes of Nitella flexilis, the reflection coefficients (σ_s) of some non-electrolytes were determined, using a zero-flow method, and were compared with those found previously on Valonia utricularis and with those obtained by Dainty and Ginzburg on other Characean internodes from transcellular osmosis experiments. The hydraulic conductivities (Lp) of the cell membranes were determined by two independent methods, that is, using hydrostatically or osmotically induced flows. From the exponential time course of P in such experiments and from the volumetric elastic modulus (ε) of the cell wall, Lp was calculated. The effect of unstirred layers in the methods described was negligibly small.In osmotic experiments with different non-plasmolysing external sucrose concentrations (20–200 mM) the exosmotic hydraulic conductivity (Lp_ex) decreases markedly with increasing concentration, while the endosmotic hydraulic conductivity (Lp_en) shows only a weak dependence. In the hydrostatic experiments the hydraulic conductivities for single cells were constant in the pressure range for P from 2 to 7 atm. In this pressure range Lp_en and Lp_ex varied for different cells from 2.2·10^?5 to 2.8·10^?5 and from 1.8·10^?5 to 2.5·10^?5 cm·s^?1·atm^?1, respectively, with an average ratio Lp_en to Lp_ex of 1.1, which indicates a polarity in water movement.These values were the same as those obtained in the osmotic experiments from extrapolation to zero sucrose concentration. At internal pressures below 2 atm the Lp-values markedly increase on approaching the plasmolytic point.The results are discussed in terms of a dehydration of the membranes (or the cytoplasm) at increased solute concentrations. In addition, the strong dependence of Lp at low internal hydrostatic pressures points to a direct influence of P on the water permeability of the membranes.     

Regulation of H+Pumping by Plant Plasmalemma under Osmotic Stress: The Role of 14-3-3 Proteins

All higher plants have high-specific sites for binding fusicoccin (FCBS), a metabolite of the fungus Fusicoccum amygdaliDel. These sites are localized on the plasmalemma and produced by the association of the dimers of 14-3-3 proteins with the C-terminal autoinhibitory domain of H⁺-ATPase. Considering the fusicoccin binding to the plasmalemma as an index characterizing the formation of this complex, we studied the influence of osmotic stress on the interaction between 14-3-3 proteins and H⁺-ATPase in the suspension-cultured sugar beet cells and protoplasts obtained from them. An increase in the osmolarity of the extracellular medium up to 0.3 Osm was shown to enhance proton efflux from the cells by several times. The number of FCBS in isolated plasma membranes increased in parallel, whereas 14-3-3 proteins accumulated in this membrane to a lesser degree. The amount of H⁺-ATPase molecules did not change, and the ATP-hydrolase activity changed insignificantly. The data obtained indicate that osmotic stress affects H⁺-ATPase pumping in the plasmalemma through its influence on the coupling between H⁺-transport and ATP hydrolysis; 14-3-3 proteins are involved in this coupling. The interaction between the plasmalemma and the cell wall is suggested to be very important in this process.