The formation and properties of thin lipid membranes from HK and LK sheep red cell lipids

Lipids were obtained from high potassium (HK) and low potassium (LK) sheep red cells by sequential extraction of the erythrocytes with isopropanol-chloroform, chloroform-methanol-0.1 M KCl, and chloroform. The extract contained cholesterol and phospholipid in a molar ratio of 0.8:1.0, and less than 1% protein contaminant. Stable thin lipid membranes separating two aqueous compartments were formed from an erythrocyte lipid-hydrocarbon solution, and had an electrical resistance of ∼10⁸ ohm-cm² and a capacitance of 0.38–0.4 µf/cm². From the capacitance values, membrane thickness was estimated to be 46–132 A, depending on the assumed value for the dielectric constant (2.0–4.5). Membrane voltage was recorded in the presence of ionic (NaCl and/or KCl) concentration gradients in the solutions bathing the membrane. The permeability of the membrane to Na⁺, K⁺, and Cl^- (expressed as the transference number, T _ion) was computed from the steady-state membrane voltage and the activity ratio of the ions in the compartments bathing the membrane. T _Na and T _K were approximately equal (∼0.8) and considerably greater than T _Cl (∼0.2). The ionic transference numbers were independent of temperature, the hydrocarbon solvent, the osmolarity of the solutions bathing the membranes, and the cholesterol content of the membranes, over the range 21–38°C. The high degree of membrane cation selectivity was tentatively attributed to the negatively charged phospholipids (phosphatidylethanolamine and phosphatidylserine) present in the lipid extract.     

Caffeine and excitation-contraction coupling in the guinea pig taenia coli

The effects of caffeine (0.2–10 mM) on the electrical and mechanical activities of guinea pig taenia coli were investigated with the double sucrose-gap method. Caffeine evoked a small tension with a latency of 20–30 sec, then phasic contraction developed and finally relaxation. The initial tension development also appeared in the Na-free solution without any marked changes in the membrane potential and membrane resistance. The phasic contraction disappeared in the Na-free solution. The relaxation in the presence of caffeine was accompanied by depolarization block of the spike generation. The minimum concentration of Ca ion needed to evoke the tension development by the caffeine was 10^-7 M. Caffeine also potentiated the twitch tension below a concentration of 5 mM either in the Na-free solution or at low temperature (5°C). NO₃ ^- and Br^- showed a similar response to caffeine on the potentiation of the twitch tension at low temperature.     

Effect of peptide PV on the ionic permeability of lipid bilayer membranes

This paper reports the effects of peptide PV (primary structure: cyclo-(D-val-L-pro-L-val-D-pro)_δ) on the electrical properties of sheep red cell lipid bilayers. The membrane conductance (G_m) induced by PV in either Na⁺ or K⁺ medium is proportional to the concentration of PV in the aqueous phase. The PV concentration required to produce a comparable increase in G_m in K⁺ medium is about 10⁴ times greater than for its analogue, valinomycin (val). Although the selectivity sequence for PV and val is similar, K⁺ ≳ Rb⁺ > Cs⁺ > NH₄ ⁺ > TI⁺ > Na⁺ > Li⁺; the ratio of GGm in K⁺ to that in Na⁺ is about 10 for PV compared to > 10³ for val. When equal concentrations of PV are added to both sides of a bilayer, the membrane current approaches a maximum value independent of voltage when the membrane potential exceeds 100 mV. When PV is added to only one side of a bilayer separating identical salt solutions of either Na⁺ or K⁺ salts, rectification occurs such that the positive current flows more easily away rather than toward the side containing the carrier. Under these conditions, a large, stable, zero-current potential (VVm) is also observed, with the side containing PV being negative. The magnitude of this VVm is about 90 mV and relatively independent of PV concentration when the latter is larger than 2 Times; 10^–5 M. From a model which assumes that V_m equals the equilibrium potential for the PV-cation complexes (MS ⁺) and that the reaction between PV and cations is at equilibrium on the two membrane surfaces, we compute the permeability of the membrane to free PV to be about 10^–5 cm s^–1, which is about 10^–7 times the permeability of similar membranes to free val. This interpretation is supported by the fact that the observed values of V_m are in agreement with the calculated equilibrium potential for MS⁺ over a wide range of ratios of concentrations of total PV in the two bathing solutions, if the unstirred layers are taken into account in computing the MS⁺ concentrations at the membrane surfaces.     

On the origin of the bioelectrical potential gverated by the freshwater clam mantle

Mantles from freshwater clams develop potential differences (PD''s) between the two surfaces when they are bathed in vitro with artificial saline solutions. The magnitude and polarity of the PD is dependent on [Ca²⁺] in the solution bathing the mantle''s shell surface. When the solutions are gassed with 5% CO₂ in oxygen, the PD is in the range 25 to 50 mv, shell side positive. It decreases if [Ca²⁺] in the shell solution is elevated. The concentration dependence is logarithmic with a slope of about -27 mv per 10-fold change in [Ca²⁺], slightly less than predicted by the Nernst equation for a membrane acting as a calcium electrode. Analysis of the electrical behavior both in intact mantles and in isolated epithelia indicates that most of the PD develops across the external membranes of epithelial cells on the shell side. There is no evidence that an active calcium transport system is involved in electrogenesis, and a model based on calcium diffusion across a selectively permeable membrane can explain existent data. If CO₂ is absent, the mantle PD is very small (2–10 mv), but still sensitive to change in external [Ca²⁺]. It is proposed that CO₂ alters intracellular pH, thereby changing the equilibrium between a large store of nonionized calcium and [Ca²⁺] in the cells. A role for carbonic anhydrase in the CO₂ effect is suggested by the action of a specific inhibitor of this enzyme. The diffusion model predicts that increasing ionized calcium should increase the PD as is actually observed. Some implications of this system for the physiology of calcium movement in vivo are discussed.     

The effect of valinomycin on the electrical properties of solutions of red cell lipids in n-decane

This paper reports the electrical properties of thick lipid membranes in the absence and presence of valinomycin. The thick lipid membranes were formed by placing a solution of sheep red cell lipids in decane between two cellophane partitions which formed the interfaces between the membrane and the two aqueous bathing solutions. The DC electrical resistance of these structures was found to be directly proportional to the reciprocal of the concentration of lipids in the decane (C_L). The limiting resistance, as (C_L ^-1) approached zero, was 3 x 10⁸ ohm-cm². Resistance was also found to be linearly related to membrane thickness. The limiting resistance at zero thickness was again 1–3 x 10⁸ ohm-cm². These data are interpreted to indicate that the DC resistance of thick lipid membranes comprises two surface resistances (R_S) at each interface with the aqueous bathing solutions, and a bulk resistance (R_B) of the lipid-decane solution, arranged in series. Measurements of the effect of variations of area on resistance were consistent with this interpretation. Valinomycin reduced R_S but had no effect on R_B. Under certain conditions, thick lipid membranes containing valinomycin behaved like highly selective K⁺ electrodes.     

The penetration of sodium into the epithelium of the frog skin

The aim of this paper is twofold. First, to describe a method for the measurement of the unidirectional flux of Na from the outer bathing solution into epithelium (J_OT), and second, to describe the use of this method under a variety of experimental conditions in order to obtain some insight into the nature of this flux. The method developed is based on the exposure of a frog skin to a Ringer solution containing ²²Na. The exposure is made so that neighboring points along the surface remain in contact with the ²²Na solution for gradually longer periods, ranging from 0 to 46 sec. Some 8 to 10 samples of the exposed part are used to obtain the time course of the uptake of ²²Na and this time course is used, in turn, to evaluate J_OT. This flux is then studied in skins mounted between two identical Ringer solutions with 115 mM Na (11.25 ± 0.10 [18] µmole·hr^-2 cm^-2), and in skins mounted with Ringer with 1 mM Na on the outside and 115 mM Na on the inside (0.43 ± 0.05 [18] µmole·hr^-1·cm^-2. From the observations that the flux is much larger than the net Na flux across the whole skin, that it is inhibited by K⁺, and is unaffected by ouabain, it is concluded that the penetration of Na⁺ into the epithelium does not occur by simple diffusion and is not directly dependent on an ouabain-sensitive mechanism. In the course of these experiments it was observed that when the skin was crushed between two chambers the uptake of Na in the neighboring exposed areas was decreased.     

Sodium flux in the smooth muscle of frog stomach

Sodium efflux from rings of frog stomach muscle was measured at 5° and 15°C in three different steady states. After incubation in normal, K-free, or ouabain (10^-4 M) solutions, intracellular cations stabilized at markedly differing levels. At 5°C, inhibition of Na extrusion was shown in the rate coefficients for ²²Na efflux, which were slightly smaller in K-free than in normal solutions, and much smaller in ouabain. Due to the intracellular Na concentration differences, total Na efflux was similar in K-free and ouabain solutions, and only ⅕ as large in normal solution. At 15°C, normal total Na flux was only 1/7;–1/10 inhibitors, and may be underestimated. The total flux differences may involve dependence of the Na pump and Na permeation on internal Na concentration. The Q ₁₀ of the steady-state fluxes was 3.7 in ouabain, 2.8 in K-free solution, and 1.9 in normal solution. The high temperature dependence of influx as well as efflux suggests transport mechanisms other than simple diffusion. Sodium turnover in the cell water was 46–66 mM/hr in inhibitors at 15°C, and a high rate of Na extrusion in normal muscle is suggested. However, cell volume:surface ratio is only 1.6 µ and all estimates of Na flux were under 3 pmoles/cm² per sec, indicating low Na permeability.     

Mechanical threshold as a factor in excitation-contraction coupling

I^-, CH₃SO₄ ^-, and ClO₄ ^-, like other previously studied type A twitch potentiators (Br^-, NO₃ ^-, SCN^-, and caffeine), lower the mechanical threshold in K depolarization contractures of frog skeletal muscle. In potentiated twitches, I^-, Br^-, CH₃SO₄ ^-, ClO₄, and SCN, as already reported for NO₃ ^- and caffeine, slightly shorten the latent period (L) and considerably increase the rate of tension development (dP/dt) during the first few milliseconds of the contraction period. Divalent cations (8 mM Ca²⁺, 0.5–1.0 mM Zn²⁺ and Cd²⁺) raise the mechanical threshold of contractures, and correspondingly affect the twitch by depressing the tension output, increasing L, and decreasing the early dP/dt, thus acting oppositely to the type A potentiators. These various results form a broad, consistent pattern indicating that electromechanical coupling in the twitch is conditioned by a mechanical threshold as it is in the contracture, and suggesting that the lower the threshold, in reference to the raised threshold under the action of the divalent cations, the more effective is a given action potential in activating the twitch as regards especially both its early rate and peak magnitude of tension development. The results suggest that the direct action by which the various agents affect the level of the mechanical threshold involves effects on E-C coupling processes of the T tubular and/or the sarcoplasmic reticulum which control the release of Ca for activating contraction.     

Hydroxyl ion movements across the human erythrocyte membrane. Measurement of rapid pH changes in red cell suspensions

A stopped flow rapid reaction apparatus capable of following changes of ±0.02 pH unit in 0.1 ml of solution in less than 0.005 sec has been developed, utilizing a commercially available pH-sensitive glass electrode. Using this instrument, extracellular pH at 37°C was followed from less than 0.025 sec to 300 sec after mixing equal volumes of the following CO₂-free solutions: (A) normal human red cells, washed three times and resuspended in 150 mM NaCl at pH 7.2 with a hematocrit of 18%; and, (B) 150 mM NaCl adjusted with HCl or NaOH to pH 2.1 to pH 10.3. A minimum of 2 ml of mixture had to flow through the electrode chamber to ensure complete washout. The mixing process produced a step change in the pH of the extracellular fluid, after which exchanges across the red cell membrane and buffering by intracellular hemoglobin caused it to return toward pH 7.2 with an approximately exponential time course. Under the assumption that pH changes after mixing represent exchanges of hydroxyl for chloride ions across the cell membrane, hydroxyl ion permeabilities (P _OH ^- in cm/sec) were calculated and found to vary from 2 x 10^-4 at pH 9 to 4 x 10^-1 at pH 4 according to the empirical relationship P _OH ^- = 170 exp (-1.51 pH). The form of the dependence of P _OH ^- on extracellular pH does not appear compatible with a simple fixed charge theory of membrane permselectivity.     

Barley beta‐glucan promotes MnSOD expression and enhances angiogenesis under oxidative microenvironment

Manganese superoxide dismutase (MnSOD), a foremost antioxidant enzyme, plays a key role in angiogenesis. Barley-derived (1.3) β-d-glucan (β-d-glucan) is a natural water-soluble polysaccharide with antioxidant properties. To explore the effects of β-d-glucan on MnSOD-related angiogenesis under oxidative stress, we tested epigenetic mechanisms underlying modulation of MnSOD level in human umbilical vein endothelial cells (HUVECs) and angiogenesis in vitro and in vivo. Long-term treatment of HUVECs with 3% w/v β-d-glucan significantly increased the level of MnSOD by 200% ± 2% compared to control and by 50% ± 4% compared to untreated H₂O₂-stressed cells. β-d-glucan-treated HUVECs displayed greater angiogenic ability. In vivo, 24 hrs-treatment with 3% w/v β-d-glucan rescued vasculogenesis in Tg (kdrl: EGFP) s843Tg zebrafish embryos exposed to oxidative microenvironment. HUVECs overexpressing MnSOD demonstrated an increased activity of endothelial nitric oxide synthase (eNOS), reduced load of superoxide anion (O₂⁻) and an increased survival under oxidative stress. In addition, β-d-glucan prevented the rise of hypoxia inducible factor (HIF)1-α under oxidative stress. The level of histone H4 acetylation was significantly increased by β-d-glucan. Increasing histone acetylation by sodium butyrate, an inhibitor of class I histone deacetylases (HDACs I), did not activate MnSOD-related angiogenesis and did not impair β-d-glucan effects. In conclusion, 3% w/v β-d-glucan activates endothelial expression of MnSOD independent of histone acetylation level, thereby leading to adequate removal of O₂⁻, cell survival and angiogenic response to oxidative stress. The identification of dietary β-d-glucan as activator of MnSOD-related angiogenesis might lead to the development of nutritional approaches for the prevention of ischemic remodelling and heart failure.     

The ionic requirements for the initiation of action potentials in insect muscle fibers

Electrical properties of locust leg muscle fibers were studied by means of intracellular electrodes. In most fibers, a depolarizing current pulse initiated a local response. A delayed decrease in membrane resistance appeared with more than about 10 mv depolarization. In some fibers a regenerative response also was found. Membrane constants were measured, applying the short cable model. The value of the space constant λ was 1.6 mm and the calculated value of R_m was about 1750 ohm cm². Action potentials could be elicited when the bathing fluid contained more than 2–5 mM Ba or Sr. Similar responses were seen with 2 mM Ca in the presence of tetraethylammonium (TEA). The overshoot of these action potentials increased with increasing [Ca⁺⁺]_o, [Sr⁺⁺]_o, or [Ba⁺⁺]_o, the increment for a 10-fold increase being about 29 mv for Ca and Sr and between 40 and 50 mv for Ba. These action potentials were inhibited by Mn ions but were not affected by tetrodotoxin or procaine. In solutions containing Ba or Sr, action potentials generated were suppressed by addition of Ca. The removal of Na ions did not change the configuration of the action potential. The results suggest that an increase in permeability to Ca, Ba, or Sr ions makes a major contribution to the initiation of action potentials in this tissue.     

Chloride Transport in Porous Lipid Bilayer Membranes

This paper describes dissipative Cl_- transport in "porous" lipid bilayer membranes, i.e., cholesterol-containing membranes exposed to 1–3 x 10^-7 M amphotericin B. P_DCl (cm·s^-1), the diffusional permeability coefficient for Cl^-, estimated from unidirectional ³⁶Cl^- fluxes at zero volume flow, varied linearly with the membrane conductance (Gm, Ω^-1·cm^-2) when the contributions of unstirred layers to the resistance to tracer diffusion were relatively small with respect to the membranes; in 0.05 M NaCl, P_DCl was 1.36 x 10^-4 cm·s^-1 when Gm was 0.02 Ω^-1·cm^-2. Net chloride fluxes were measured either in the presence of imposed concentration gradients or electrical potential differences. Under both sets of conditions: the values of P_DCl computed from zero volume flow experiments described net chloride fluxes; the net chloride fluxes accounted for ~90–95% of the membrane current density; and, the chloride flux ratio conformed to the Ussing independence relationship. Thus, it is likely that Cl^- traversed aqueous pores in these anion-permselective membranes via a simple diffusion process. The zero current membrane potentials measured when the aqueous phases contained asymmetrical NaCl solutions could be expressed in terms of the Goldman-Hodgkin-Katz constant field equation, assuming that the P_DNa/P_DCl ratio was 0.05. In symmetrical salt solutions, the current-voltage properties of these membranes were linear; in asymmetrical NaCl solutions, the membranes exhibited electrical rectification consistent with constant-field theory. It seems likely that the space charge density in these porous membranes is sufficiently low that the potential gradient within the membranes is approximately linear; and, that the pores are not electrically neutral, presumably because the Debye length within the membrane phase approximates the membrane thickness.     

Uptake of aluminium into Arabidopsis root cells measured by fluorescent lifetime imaging

Background and Aims

Measuring the Al³⁺ uptake rate across the plasma membrane of intact root cells is crucial for understanding the mechanisms and time-course of Al toxicity in plants. However, a reliable method with the sufficient spatial and temporal resolution to estimate Al³⁺ uptake in intact root cells does not exist.

Methods

In the current study, fluorescent lifetime imaging (FLIM) analysis was used to quantify Al³⁺ uptake in the root-cell cytoplasm in vivo. This was performed via the estimation of the fluorescence lifetime of Al–lumogallion {5-chloro-3[(2,4-dihydroxyphenyl)azo]-2-hydroxybenzenesulfonic acid} complexes and measurements of intracellular pH while exposing arabidopsis seedlings to acidic and Al³⁺ stresses.

Key Results

The lifetime of Al–lumogallion complexes fluorescence is pH-dependent. The primary sites for Al³⁺ entry are the meristem and distal elongation zones, while Al³⁺ uptake via the cortex and epidermis of the mature root zone is limited. The maximum rates of Al uptake into the cytoplasm (2–3 µmol m⁻³ min⁻¹ for the meristematic root zone and 3–7 µmol m⁻³ min⁻¹ for the mature zone) were observed after a 30-min exposure to 100 µm AlCl₃ (pH 4·2). Intracellular Al concentration increased to 0·4 µm Al within the first 3 h of exposure to 100 µm AlCl₃.

Conclusions

FLIM analysis of the fluorescence of Al–lumogallion complexes can be used to reliably quantify Al uptake in the cytoplasm of intact root cells at the initial stages of Al³⁺ stress.Key words: Acid stress, Al³⁺, aluminium toxicity, Arabidopsis thaliana, low pH, fluorescent lifetime imaging (FLIM), lumogallion     

Three-way Interaction between 14-3-3 Proteins, the N-terminal Region of Tyrosine Hydroxylase, and Negatively Charged Membranes

Tyrosine hydroxylase (TH), the rate-limiting enzyme in the synthesis of catecholamines, is activated by phosphorylation-dependent binding to 14-3-3 proteins. The N-terminal domain of TH is also involved in interaction with lipid membranes. We investigated the binding of the N-terminal domain to its different partners, both in the unphosphorylated (TH-(1–43)) and Ser¹⁹-phosphorylated (THp-(1–43)) states by surface plasmon resonance. THp-(1–43) showed high affinity for 14-3-3 proteins (K_d ∼ 0.5 μm for 14-3-3γ and -ζ and 7 μm for 14-3-3η). The domains also bind to negatively charged membranes with intermediate affinity (concentration at half-maximal binding S_0.5 = 25–58 μm (TH-(1–43)) and S_0.5 = 135–475 μm (THp-(1–43)), depending on phospholipid composition) and concomitant formation of helical structure. 14-3-3γ showed a preferential binding to membranes, compared with 14-3-3ζ, both in chromaffin granules and with liposomes at neutral pH. The affinity of 14-3-3γ for negatively charged membranes (S_0.5 = 1–9 μm) is much higher than the affinity of TH for the same membranes, compatible with the formation of a ternary complex between Ser¹⁹-phosphorylated TH, 14-3-3γ, and membranes. Our results shed light on interaction mechanisms that might be relevant for the modulation of the distribution of TH in the cytoplasm and membrane fractions and regulation of l-DOPA and dopamine synthesis.     

The capacitance of skeletal muscle fibers in solutions of low ionic strength

The capacitance of skeletal muscle fibers was measured by recording with one microelectrode the voltage produced by a rectangular pulse of current applied with another microelectrode. The ionic strength of the bathing solution was varied by isosmotic replacement of NaCl with sucrose, the [K] [Cl] product being held constant. The capacitance decreased with decreasing ionic strength, reaching a value of some 2 µF/cm² in solutions of 30 mM ionic strength, and not decreasing further in solutions of 15 mM ionic strength. The capacitance of glycerol-treated fibers did not change with ionic strength and was also some 2 µF/cm². It seems likely that lowering the ionic strength reduces the capacitance of the tubular system (defined as the charge stored in the tubular system), and that the 2 µF/cm² which is insensitive to ionic strength is associated with the surface membrane. The tubular system is open to the external solution in low ionic strength solutions since peroxidase is able to diffuse into the lumen of the tubules. Twitches and action potentials were also recorded from fibers in low ionic strength solutions, even though the capacitance of the tubular system was very small in these solutions. This finding can be explained if there is an action potential—like mechanism in the tubular membrane.     

Decreased K+ conductance produced by Ba++ in frog sartorius fibers

The action of Ba⁺⁺ on membrane potential (E_m) and resistance (R_m) of frog (R. pipiens) sartorius fibers was studied. In normal Cl^- Ringer''s, Ba⁺⁺ (<9 mM) did not depolarize or induce contractions, but increased R_m slightly above the control value of 3.8 ± 0.6 KΩ-cm². In Cl^--free Ringer''s (methane sulfonate) R_m was 28.8 ± 2.8 KΩ-cm², and low concentrations of Ba⁺⁺ (0.05–5.0 mM) depolarized and induced spontaneous contractions (fibrillation), even in tetrodotoxin. To stop disturbance of the microelectrodes, contractions were prevented by using two Cl^--free solutions: (a) twice hypertonic with sucrose (230 mM), or (b) high K⁺ (83 mM) partially replacing Na⁺. In the hypertonic solution, the fiber diameters decreased, E_m increased slightly, and R_m decreased to 9.0 ± 0.6 KΩ-cm² (perhaps due to swelling of sarcotubules). Ba⁺⁺ (0.5 mM) rapidly increased R_m to 31.3 ± 3.8, decreased E_m (e.g., to -30 mv), and induced spontaneous "action potentials;" Sr⁺⁺ had no effect. In the high K⁺ solution, the fibers were nearly completely depolarized, and R_m was decreased markedly to 1.5 ± 0.2 KΩ-cm²; Ba⁺⁺ increased R_m to 6.7 ± 0.5 KΩ-cm². The Ba⁺⁺ actions usually began within 0.5 min and reached a maximum within 5 min. Addition of SO₄ ⁼, to precipitate the Ba⁺⁺, rapidly reversed the increase in R_m. Ba⁺⁺ must act by decreasing K⁺ conductance (g_K). In Cl^- Ringer''s, the high g_Cl/g_K ratio masked the effect of Ba⁺⁺ on g_K. Thus, small concentrations of Ba⁺⁺ specifically and rapidly decrease g_K.     

Potassium fluxes in dialyzed squid axons

Measurements have been made of K influx in squid giant axons under internal solute control by dialysis. With [ATP]_i = 1 µM, [Na]_i = 0, K influx was 6 ± 0.6 pmole/cm² sec; an increase to [ATP]_i = 4 mM gave an influx of 8 ± 0.5 pmole/cm² sec, while [ATP]_i 4, [Na]_i 80 gave a K influx of 19 ± 0.7 pmole/cm² sec (all measurements at ∼16°C). Strophanthidin (10 µM) in seawater quantitatively abolished the ATP-dependent increase in K influx. The concentration dependence of ATP-dependent K influx on [ATP]_i, [Na]_i, and [K]_o was measured; an [ATP]_i of 30 µM gave a K influx about half that at physiological concentrations (2–3 mM). About 7 mM [Na]_i yielded half the K influx found at 80 mM [Na]_i. The ATP-dependent K influx responded linearly to [K]_o from 1–20 mM and was independent of whether Na, Li, or choline was the principal cation of seawater. Substances tested as possible energy sources for the K pump were acetyl phosphate, phosphoarginine, PEP, and d-ATP. None was effective except d-ATP and this substance gave 70% of the maximal flux only when phosphoarginine or PEP was also present.     

Coupled transport of protons and anions through lipid bilayer membranes containing a long-chain secondary amine

Summary Transport of protons and halide ions through planar lipid bilayers made from egg lecithin and a long-chain secondary amine (n-lauryl [trialkylmethyl] amine) inn-decane was studied. Net proton fluxes were measured with a pH electrode, and halide fluxes were measured with⁸²Br^– and³⁶Cl^–. In membranes containing the secondary amine, a large net proton flux was produced either by a Br^– gradient with symmetrical pH or by a pH gradient with symmetrical Br^–, but not by a pH gradient in Br^–-free solutions. This H⁺ flux was electrically silent (nonconductive), and the H⁺ permeability coefficient was >10^–3 cm sec^–1 in 0.1m NaBr. In Br^–-free solutions, H⁺ selectivity was observed electrically by measuring conductances and zero-current potentials generated by H⁺ activity gradients. The permeability coefficient for this ionic (conductive) H⁺ flux was about 10^–5 cm sec^–1, several orders of magnitude smaller than the H⁺ permeability of the electroneutral pathway. Large electroneutral Br^– exchange fluxes occurred under symmetrical conditions, and the permeability coefficient for Br^– exchange was about 10^–3 cm sec^–1 at pH 5. The one-way Br^– flux was inhibited by substituting SO ₄ ⁼ for Br^– on the trans side of the membrane. These results support a titratable carrier model in which the secondary amine exists in three forms (C, CH⁺ and CHBr). Protons can cross the membrane either as CHBr (nonconductive) or as CH⁺ (conductive), whereas Br^– crosses the membrane primarily as CHBr (nonconductive). In addition to these three types of transport, there is also a pH-dependent conductive flux of Br^– which has a permeability coefficient of about 10^–7 cm sec^–1 at pH 5. Experiments with lipid monolayers suggest that the pH dependence of this conductive flux is caused by a change in surface potential of about +100 mV between pH 9.5 and 5.0.     

Chloride-activated water permeability in the frog corneal epithelium

We have previously reported that the isolated frog corneal epithelium (a Cl^–-secreting epithelium) has a large diffusional water permeability (P_dw 1.8×10^–4 cm/s). We now report that the presence of Cl^– in the apical-side bathing solution increases the diffusional water flux, J_dw (in both directions) by 63% from 11.3 to 18.4 l min^–1 · cm^–2 with 60 mm [Cl] exerting the maximum effect. The presence of Cl^– in the basolateral-side bathing solution had no effect on the water flux. In Cl^–-free solutions amphotericin B increased J_dw by 29% but only by 3% in Cl^–-rich apical-side bathing solution, suggesting that in Cl^–-rich apical side bathing solution, the apical barrier is no longer rate limiting. Apical Br^– (75 mm) also increased J_dw by 68%. The effect of Cl^– on J_dw was observed within 1 min after its addition to the apicalside bathing solution. HgCl₂ (0.5 mm) reduced the Cl^–-increased P_dw by 31%. The osmotic permeability (P_f) was also measured under an osmotic gradient yielding values of 0.34 and 2.88 (x 10^–3 cm/s) in Cl^–-free and Cl^–-rich apical-side bathing solutions respectively. It seems that apical Cl^–, or Cl^– secretion into the apical bath could activate normally present but inactive water channels. In the absence of Cl^–, water permeability of the apical membrane seems to be limited to the permeability of the lipid bilayer.This work was supported by National Eye Institute grants EY-00160 and EY-01867.