Transfer of sodium ions across the erythrocyte membrane in manic — Depressive illness: Treatment with lithium carbonate

The efflux of ²²Na from erythrocytes was measured $\text{in vitro}$ under experimental conditions such that rate constants due to efflux either by active transport, passive diffusion, or exchange diffusion could be calculated. No significant differences were found in the rate constants for ²²Na efflux between seven male bipolar depressed patients and eight male control subjects, who had no personal or family history of psychiatric illness. Treatment of patients with lithium carbonate either for less than one week or for 4–5 weeks produced no changes in the rate constants describing the efflux of ²²Na from red cells. Also, addition of 1mM LiCl $\text{in vitro}$ did not alter the active transport of ²²Na from erythrocytes. These data provide no evidence for either an abnormality in ²²Na transfer across the red cell membrane of bipolar depressives or an effect of the lithium ion upon such transfer.     

Effects of pH on β-hydroxybutyrate transport in rat erythrocytes and thymocytes

Entry of β-hydroxybutyrate into erythrocytes and thymocytes is facilitated by a carrier (C), as judged from temperature dependence, saturation kinetics, stereospecificity, competition with lactate and pyruvate, and inhibition by moderate concentrations of methylisobutylxanthine, phloretin, or α-cyanocinnamate. We studied the dependence of influx and efflux on internal and external pH and [β-hydroxybutyrate]. Lowering external pH from 8.0 to 7.3 to 6.6 enhanced influx into erythrocytes by lowering entry $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ from 29 to 16 to 10 mM, entry $\text{V}$ being independent of external pH. Lowering external pH inhibited efflux. At low external pH, external β-hydroxybutyrate enhanced efflux slightly. At high external pH, external β-hydroxybutyrate inhibited efflux. Internal acidification inhibited influx and internal alkalization enhanced influx. Internal β-hydroxybutyrate (βHB) enhanced influx more in acidified than alkalized cells. These data are compatible with coupled βHB^?/OH^? exchange, βHB^? and OH^? competing for influx, C : OH^? moving faster than C : βHB^?, empty C being immobile. They are also compatible with coupled βHB^?/H⁺ copermeation, empty C moving inward faster than H⁺ : C : βHB^?, H⁺ : C being immobile, and C : βHB^? (without H⁺) being so unstable as not to be formed in significant amounts (relative to C, H⁺ : C, and H⁺ : C : βHB^?).     

The effect of pH on α-methyl-d-glucoside accumulation by rat kidney cortex slices

The kinetics of α-methyl-d-glucoside accumulation by rat kidney cortex slices under conditions of varying extracellular pH are compared with values obtained at pH 7.4. At pH below 7.4 there is a diminished initial uptake and reduced influx of the sugar which results in a decrease in the steady-state intracellular pool. This was associated with a decrease in the $\text{V}$ of the entry process without affecting the apparent $\text{K}{}_{\mathrm{m}}$ of transport. At pH 8 there is no change in the rate of glucoside entry. The efflux of the glucoside, however, is impaired and the steady-state concentration gradient becomes greater than that observed at pH 7.4.     

Role of the plasma membrane in the mechanism of cholesterol efflux from cells

In order to investigate the role of the plasma membrane in determining the kinetics of removal of cholesterol from cells, the efflux of [³H]cholesterol from intact cells and plasma membrane vesicles has been compared. The release of cholesterol from cultures of Fu₅AH rat hepatoma and WIRL-3C rat liver cells to complexes of egg phosphatidylcholine (1 mg / ml) and human high-density apolipoprotein is first order with respect to concentration of cholesterol in the cells, with half-times ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$) for at least one-third of the cell cholesterol of 3.2 ± 0.6 and 14.3 ± 1.5 h, respectively. Plasma membrane vesicles (0.5–5.0 μm diameter) were produced from both cell lines by incubating the cells with 50 mM formaldehyde and 2 mM dithiothreitol for 90 min. The efflux of cholesterol from the isolated vesicles follows the same kinetics as the intact, parent cells: the $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ values for plasma membrane vesicles of Fu₅AH and WIRL cells are 3.9 ± 0.5 and 11.2 ± 0.7 h, respectively. These $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ values reflect the rate-limiting step in the cholesterol efflux process, which is the desorption of cholesterol molecules from the plasma membrane into the extracellular aqueous phase. The fact that intact cells and isolated plasma membranes release cholesterol at the same rate indicates that variations in the plasma membrane structure account for differences in the kinetics of cholesterol release from different cell types. In order to investigate the role of plasma membrane lipids, the kinetics of cholesterol desorption from small unilamellar vesicles prepared from the total lipid isolated from plasma membrane vesicles of Fu₅AH and WIRL cells were measured. Half-times of cholesterol release from plasma membrane lipid vesicles of Fu₅AH and WIRL cells were the same, with values of 3.1 ± 0.1 and 2.9 ± 0.2 h, respectively. Since bilayers formed from isolated plasma membrane lipids do not reproduce the kinetics of cholesterol efflux observed with the intact plasma membranes, it is likely that the local domain structure, as influenced by membrane proteins, is responsible for the differences in $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ values for cholesterol efflux from these cell lines.     

The characterization of energized and partially de-energized (respiration-independent) β-galactoside transport into escherichia coli

Unidirectional fluxes of [¹⁴C]lactose by whole cells of Escherichia coli under highly energized and partially de-energized (in the presence of CN^?) conditions are analyzed kinetically.When the cells are energized, the value for $\text{V}$ influx is $\text{0.45 ± 0.01}\text{mM}$ internal concentration increment/s and $\text{K}{}_{\mathrm{t}}$ is $\text{0.26 ± 0.03}\text{mM}$. At an external concentration of 0.61 mM the steady-state internal concentration is 0.25 M, reached after about 1h. The maximum steady-state concentration ratio is $\text{2 · 10}{}^3$.The efflux process under these conditions is non-saturable, being linearly dependent upon internal concentration over the range 25–250 mM with a first-order rate constant of $\text{8.8 ± 0.2 · 10}{}^{\mathrm{?4}}\text{s}{}^{\mathrm{?1}}$.The transport in the presence of CN^? is active, with a maximum concentration ratio (internal concentration/external concentration) of 104, and the uptake is mimicked by anoxia (< 70 ppm O₂).The effects of CN^? are to lower the $\text{V}$ for influx and to change the efflux from a non-saturable to a saturable process with a value for $\text{K}{}_{\mathrm{t}}$ (60 mM) intermediate between that for energized efflux ($\text{> 250}\text{mM}$) and influxe (0.3–0.6 mM), the latter value not changing appreciably. Partial de-energization thus affects both the influx and efflux processes.     

R-factor-mediated resistance to tetracycline in Escherichia coli K12: An R-factor with a mutation to temperature-sensitive tetracycline resistance

R-factor-mediated resistance to tetracycline was studied in $\text{Escherichia coli}$ K12 carrying an $\text{fi}{}^{\mathrm{+}}$ F-like R-factor which has a mutation resulting in temperature-sensitive resistance to the drug. The rate of uptake of tetracycline in this mutant is sensitive to temperature, but the rate of efflux is not. These results are consistent with the view that resistance to tetracycline is expressed at the level of the influx rather than of the efflux of tetracycline.     

Factors affecting the relative magnitudes of the ouabain-sensitive and the ouabian-insensitive fluxes of thallium ion in erythrocytes

A maximal rate of the ouabain-sensitive ²⁰⁴Tl influx in human erythrocytes can be attained at trace concentrations of Tl⁺ in Mg²⁺ isotonic media free of K⁺ and Na⁺. The maximal influx of Tl⁺ from isotonic Mg(NO₃)₂ at 20°C and pH 7.4 was $\text{0.45}\text{mM}\text{· 1}{}^{\mathrm{?1}}\text{· h}{}^{\mathrm{?1}}$ with a $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ of 0.025 mM. In contrast to the active influx of Tl⁺, the passive Tl⁺ fluxes were neither saturated nor influenced by external cations in the range of concentrations of Tl⁺ and K⁺ studied. The rate constants of Tl⁺ passive fluxes in human and cat erythrocytes can be related to pH by the equation $\text{log}\text{k}{}_{\mathrm{<mtext>in(out)</mtext>}}\text{= –A + B ·}\text{pH}$, where $\text{A}$ and $\text{B}$ are empirical constants for particular conditions. The apparent activation energy was 16 and 11 kcal/mol in sulphate and nitrate media, respectively. Tl⁺ and the alkali metal cations seem to overcome a common barrier in the erythrocyte membrane. Nevertheless, the rate of the passive penetration of Tl⁺ is about two orders of magnitude faster than those of K⁺ or Rb⁺. An extra non-Coulombic interaction between Tl⁺ and membrane ligands appears to be involved providing an accumulation of Tl⁺ somewhere in the vicinity of the membrane barrier and increasing the diffusion fluxes of Tl⁺ in both directions.     

Effect of acetazolamide on sodium transport through the isolated frog skin at low and high external sodium concentrations.

The action of acetazolamine on sodium transport in $\text{Rana esculenta}$ skin was studied with the external face bathed in dilute (2mMM) or concentrated (Ringer) solutions of sodium chloride.The absorption of Na⁺ from a dilute solution is inhibited at an acetazolamide concentration of 10⁻⁵M. This is due to an inhibition of the influx: the efflux remains unchanged. Acetazolamide has no effect, however, on transport from Ringer solution.The graphic determination of the Na⁺ transport pool at the 2 mM NaCl concentration showed that acetazolamide diminished the pool without affecting the $\text{t}\text{1}\text{2}$. The inhibitor had no effect on the pool at the higher (Ringer) concentration.These results indicate that acetazolamide acts on the external barrier of the sodium transport compartment without affecting the active pump of this ion when it is being transported from a dilute sodium chloride solution.     

Kinetics of sulfate uptake by yeast

Uptake of sulfate by yeast requires the presence of a metabolic substrate and is dependent on the time during which the cells have been metabolizing in the absence of sulfate. At low concentrations of sulfate, uptake can be described by simple saturation kinetics. Uptake of sulfate is accompanied by a net proton influx of 3 H⁺ and an efflux of 1 K⁺ for each sulfate ion taken up. Divalent cations stimulate sulfate uptake at low concentrations of sulfate; the maximal rate of uptake is not significantly affected but $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ is lowered. Stimulation by divalent cations shows an optimum at a cation concentration of about 4 mM. Monovalent cations are less effective, trivalent cations are more effective in stimulating sulfate uptake. The results are qualitatively in accordance with the notion, that the effect of cations is due to an effect via the surface potential.     

Rapid alteration in Ca++ content and fluxes in phorbol 12-myristate 13-acetate treated myoblasts

The tumor promoter phorbol 12-myristate 13-acetate rapidly induces alterations in both Ca⁺⁺ content and transport in cultured differentiated chick myoblasts. At 4 ng/ml (6nM), the promoter caused a 25 ± 12% decrease in total intracellular Ca⁺⁺ within 5 h after its addition. Measurement of ⁴⁵Ca⁺⁺ transport at this time revealed a 15 ± 6% decrease in the rate constants for both efflux and influx. Values of $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ for the cytosolic Ca⁺⁺ pool in control and treated cells were 9.1 and 10.7 min, respectively, for efflux and 8.6 and 10.4 min, respectively, for influx. Ca⁺⁺ influx was decreased maximally within 90 sec after promoter addition. No effect was observed on ⁸⁶Rb⁺ uptake or intracellular concentration at equilibrium. The Ca⁺⁺ response is among the most rapid yet reported and may play a primary role in altering cellular metabolism.     

A second mechanism for sodium extrusion in Halobacterium halobium: a light-driven sodium pump.

Membrane vesicles from a red mutant of $\text{Halobacterium}\text{halobium}$ R₁ accumulate protons when illuminated causing the pH of the suspension to rise. Sodium is extruded from the vesicles and a membrane potential is formed. This potential and the proton uptake are abolished by valinomycin if K⁺ is present. In contrast, Na⁺-efflux is uninhibited by valinomycin even though no membrane potential is detectable and H⁺ influx does not occur. $\text{Bis}$ (hexafluoracetonyl)acetone (1799) stimulates proton uptake but does not abolish membrane potential. We propose that a light-dependent sodium pump is present. Passive proton uptake occurs in response to the electrical gradient created by this light-driven Na⁺ pump in contrast to the $\text{active}$ proton, and passive Na⁺ flux that occurs in response to the light-driven proton pump described in vesicles of the parent strain of $\text{H.}\text{halobium}$ R₁.     

The basic asymmetry of Na+-dependent glycine transport in Ehrlich cells

Influx and efflux of glycine have been examined as a function of external and internal Na⁺ concentrations, respectively, when $\text{Δ}\text{μ}{}_{\mathrm{<mtext>Na</mtext>}}\text{= 0}$. With $\text{Δ}\text{μ}{}_{\mathrm{<mtext>Na</mtext>}}\text{= 0}$ it was found that at comparable external and cellular Na⁺ levels, the $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for efflux was larger by an order of magnitude than the value for influx and the $\text{V}$ for efflux was several times greater than the $\text{V}$ for influx. For both fluxes the major effect of Na⁺ was to decrease the $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ value. The observations are consistent with the conclusion that the Na⁺-dependent transport system is asymmetric per se. Influx and efflux of glycine were increased in a near linear manner by increasing the Na⁺ concentration from 13 to 100 mM, the half-time for glycine equilibration being a function of the Na⁺ concentration in absence of an electrochemical potential difference for Na⁺. In Na⁺-free media ($\text{[}\text{Na}{}^{\mathrm{+}}\text{] < 5}\text{mM}$) equilibration of glycine between cells and medium was not achieved after 60 min at 25°C. With $\text{Δ}\text{μ}{}_{\mathrm{<mtext>Na</mtext>}}\text{= 0}$, efflux (or uptake) of glycine was not affected by internal (or external) K⁺ between 20 and 120 mM suggesting that K⁺ plays no direct role in Na⁺-dependent transport of glycine in Ehrlich cells.     

Cotransport of phosphate and sodium by yeast

Phosphate uptake by yeast at pH 7.2 is mediated by two mechanisms, one of which has a $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ of 30 μM and is independent of sodium, and a sodium-dependent mechanism with a $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ of 0.6 μM, both $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ values with respect to monovalent phosphate. The sodium-dependent mechanism has two sites with affinity for Na⁺, with affinity constants of 0.04 and 29 mM. Also lithium enhances phosphate uptake; the affinity constants for lithium are 0.3 and 36 mM. Other alkali ions do not stimulate phosphate uptake at pH 7.2. Rubidium has no effect on the stimulation of phosphate uptake by sodium.Phosphate and arsenate enhance sodium uptake at pH 7.2. The $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ of this stimulation with regard to monovalent orthophosphate is about equal to that of the sodium-dependent phosphate uptake.The properties of the cation binding sites of the phosphate uptake mechanism and those of the phosphate-dependent cation transport mechanism have been compared. The existence of a separate sodium-phosphate cotransport system is proposed.     

Strophanthidin-sensitive components of potassium and sodium movements in skeletal muscle as influenced by the internal sodium concentration

"Low sodium" muscles were prepared which contained around 5 mmoles/kg fiber of intracellular sodium. "High sodium" muscles containing between 15 and 30 mmoles/kg fiber of intracellular sodium were also prepared. In low sodium muscles application of 10^-5 M strophanthidin reduced potassium influx by about 5%. Potassium efflux was unaffected by strophanthidin under these conditions. In high sodium muscles, 10^-5 M strophanthidin reduced potassium influx by 45% and increased potassium efflux by 70%, on the average. In low sodium muscles sodium efflux was reduced by 25% during application of 10^-5 M strophanthidin while in high sodium muscles similarly treated, sodium efflux was reduced by about 60%. Low sodium muscles showed a large reduction in sodium efflux when sodium ions in the Ringer solution were replaced by lithium ions. The average reduction in sodium efflux was 4.5-fold. Of the amount of sodium efflux remaining in lithium. Ringer''s solution, 40% could be inhibited by application of 10^-5 M strophanthidin. The total sodium efflux from low sodium muscles exposed to Ringer''s solution in which lithium had been substituted for sodium ions for a period of 1 hr can be fractionated as 78% Na-for-Na interchange, 10% strophanthidin-sensitive sodium pump, and 12% residual sodium efflux. It is concluded that large strophanthidin-sensitive components of sodium and potassium flux can be expected only at elevated sodium concentrations within the muscle cells.     

Reduced immunoglobulin G activates complement system with decreased cooperativity

Sheep erythrocytes sensitized with intact antibody or reduced and alkylated antibody were lysed by guinea-pig serum indicating that reduced and alkylated antibody bound and activated complement. Reduction of antibody caused erythrocyte lysis to exhibit pseudo-first-order kinetics, while the lysis kinetics of erythrocytes sensitized with intact antibody was sigmoidal. Analysis of erythrocyte lysis by complement according to the von Krogh equation showed that reduction of antibody diminished the von Krogh exponent $\text{n}$ from 2.8 to 1.3, while the value of $\text{K}$ remained unchanged at 0.17 (complement dilution). These observations suggested that the sole effect of the reduction of antibody inter-heavy-chain and heavy-light chain disulfide bonds was to diminish the cooperativity of antibody-complement interaction.     

Developmental changes in membrane transport and permeability in the early mouse embryo

Electrophysiological and isotope tracer flux experiments were performed to measure the membrane ion permeability and transport properties of the two-cell mouse embryo. The results show that the internal exchangeable Na and K are 151 and 130 mM, respectively, and their membrane permeabilities are (P_Na) 16 × 10^?8 cm sec^?1 and (P_K) 21 × 10^?8 cm sec^?1. These values predict a membrane potential of ?24 mV (inside negative) which agrees well with ?19 mV measured with microelectrodes. Ouabain-sensitive isotope fluxes demonstrate a Na/K pump mechanism with a stoichiometry of 1.7:1 (Na:K). An external-Na-dependent Na efflux is demonstrated by the reduction of unidirectional Na efflux in Na-free medium, but there is no evidence for a similar mechanism of K efflux at this stage of development. These results are compared with the values reported for the mouse oocyte [Powers, R. D., and Tupper, J. T. (1974). Develop. Biol.38, 320–331; (1975). Exp. Cell Res.91, 413–421]. The hyperpolarization of the membrane potential as compared with the oocyte (?13 mV) results primarily from the increased $\text{P}{}_{\mathrm{<mtext>K</mtext>}}\text{P}{}_{\mathrm{<mtext>Na</mtext>}}$ ratio. A similar phenomenon has been noted in other developing embryos. The increase in pump-mediated K influx at the two-cell stage is accompanied by a decrease of similar magnitude in the external-K-dependent K efflux which is found in the oocyte. This suggests that the KK exchange mechanism may be converted to an active pump. Because of the changes in ion concentrations and movements and the unusual metabolic requirements of the mouse embryo, the effect of external Na on the uptake of glucose and pyruvate in the oocyte and two- and eight-cell stage was examined. No Na-dependent carbohydrate transport could be found at these stages.     

Effect of pH, carbamylation and other hemoglobins on deoxyhemoglobin S aggregation inside intact erythrocytes as detected by proton relaxation rate measurements.

Measurement of the transverse water proton relaxation rate has been used to study the effect of pH, carbamylation, and other hemoglobins on the aggregation of deoxyhemoglobin S inside intact erythrocytes. Upon complete deoxygenation, cyanate-treated ($\text{S}\text{S}$) erythrocytes and erythrocytes heterozygous with respect to hemoglobin S ($\text{A}\text{S}$, $\text{C}\text{S}$, and $\text{S}\text{D}$) have high transverse water proton relaxation rates very similar to the values obtained with homozygous ($\text{S}\text{S}$) erythrocytes. These results suggest extensive intermolecular interactions between deoxyhemoglobin S molecules and a resultant increase in the correlation time for the small fraction of “irrotationally bound” water. When the transverse relaxation rate in deoxygenated ($\text{S}\text{S}$) erythrocytes was measured as a function of pH, the maximum rate was observed between pH 7.0 and 7.5. Upon increasing the pH beyond this range the observed relaxation rate decreases as does the number of sickled cells. Upon decreasing the pH, the observed transverse relaxation rate also decreases but the ratio of values from $\text{deoxy}\text{oxy}$ ($\text{S}\text{S}$) erythrocytes remains in the normal range of 4–6 and the number of sickled cells does not change. Therefore, the deoxyhemoglobin S aggregate inside sickled erythrocytes, as observed by water proton relaxation rates, is not altered by carbamylation or by the presence of nongelling hemoglobins. In addition, the enhancement of the relaxation rates as a function of pH is consistent with the number of sickled forms observed.     

Developmental changes of glycine transport in the dog

The renal clearance of amino acids was measured in canine pups between 5 days and 12 weeks of age. The reabsorption of glycine was incomplete at 5 and 21 days, indicating a physiologic aminoaciduria of immaturity. An adult pattern of 97–100% reabsorption appeared by 8 weeks of age. The uptake of glycine by isolated renal tubules from 5-day-old, 3-month-old and adult dogs was examined towards an understanding of the events underlying this aminoaciduria. The initial uptake of 0.042 mM glycine by isolated tubules from the newborn was lower than that of the adult, but after 30 min of incubation the newborn surpassed the adult. A steady state of uptake was not achieved by the newborn even after 90 min of incubation, while it was achieved in the adult after 30 min. The uptake by the 3-month-old tubules resembled the adult at the early time points and the newborn at later points. With 1.032 mM glycine, a similar relationship of uptake between adult and newborn tubules was found, except with this concentration, the uptake by both the newborn and adult tubules reached a steady state. The concentration dependence of glycine uptake showed two saturable transport systems with similar apparent $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ and $\text{V}{}_{\mathrm{<mtext>max</mtext>}}$ values after 30 min of incubation for all three age groups. Determination of glycine flux by compartmental analysis revealed decreased influx and efflux in the newborn, but with a greater decrease in efflux, compared to adult. These changes of influx and efflux which accompany renal tubule maturation could contribute to the increased intracellular amino acid levels and decreased reabsorption of amino acids seen in the immature dog.     

Characterization of calcium liberation from a human platelet membrane fraction

Calcium efflux and EGTA-induced calcium release from an internal platelet membrane fraction have been studied after the oxalate-supported calcium uptake had reached steady state. Increasing external calcium concentrations stimulate the calcium efflux velocity, with an apparent half-maximal stimulation at about 5 μM outside calcium concentration and a maximal velocity of calcium efflux of $\text{4.66 ± 2.32}\text{nmol}\text{·}\text{min}{}^{\mathrm{?1}}\text{·}\text{mg}{}^{\mathrm{?1}}$. Moreover, the ratio of the liberated calcium on the loaded calcium seems to be independent of the increasing external calcium concentration. Increasing the calculated internal calcium concentration by varying the oxalate potassium concentration from 10 mM to 1 mM results in an increase of the liberated calcium from the membrane vesicles from 7.4% to 63%, respectively, without changing the calcium efflux velocity. Similar conclusions can be drawn from the observation of results from the calcium efflux and EGTA-induced calcium release methods. Moreover, calcium pump reversal does not seem to be responsible for the calcium efflux or calcium release. All these different points added to the previously described regulation of calcium efflux by the catalytic subunit of cAMP protein kinase suggest us that the mechanism of calcium liberation by the platelet membranes is different from the calcium uptake.     

Light-driven sodium transport in sub-bacterial particles of Halobacterium halobium

Light-induced Na⁺ efflux was observed in sub-bacterial particles of Halobacterium halobium loaded and suspended in 4 M NaCl solution. The Na⁺ efflux was not ATP driven, since ATPase inhibitors were without effect or even enhanced efflux at low light intensity. Uncouplers, on the other hand, inhibited Na⁺ efflux, the inhibition being complete at low light intensity. The Na⁺ efflux was accompanied by proton influx. Both processes were dependent on light intensity, unaffected or enhanced by ATPase inhibitors and similarly affected by uncouplers. Proton influx was not observed in particles loaded with 4 M KCl instead of 4 M NaCl. Na⁺ transport in the dark could be induced by artificial formation of a pH difference across the membrane; changing the sign of the pH difference reversed the direction of the Na⁺ transport. Proton influx in the dark followed the artificial formation of a sodium gradient ($\text{[Na}{}^{\mathrm{+}}\text{]}{}_{\mathrm{in}}\text{> [Na}{}^{\mathrm{+}}\text{]}{}_{\mathrm{out}}$). These results may be explained by a Na⁺/H⁺ antiport mechanism. The fluxes of Na⁺ and H⁺ were of comparable magnitude, but the initial rate of Cl^? efflux in the same experiment was one-third of the initial rate of Na⁺ efflux. Consequently Cl^? is not regarded as a participant in the Na⁺ efflux mechanism.