Voltage dependent potassium fluxes and the significance of action potentials in Acetabularia

Membrane potential, V_m, and K⁺(⁸⁶Rb⁺) fluxes have been measured simultaneously on individual cells of Acetabularia mediterranea. During resting state (resting potential approx. ?170 mV) the K⁺ influx amounts to 0.24–0.6 pmol · cm^?2 · s^?1 and the K⁺ efflux to 0.2–1.5 pmol · cm^?2 s^?1. According to the K⁺ concentrations inside and outside the cell (40 : 1) the voltage dependent K⁺ flux (zero at V_m = E_K = ?90 mV) is stimulated approx. 40-fold for V_m more positive than E_K.It is calculated that during one action potential (temporary depolarization to V_m more positive than E_K) a cell looses the same amount of K⁺, which leaks in during 10–20 min in the resting state (V_m = ?170 mV). Since action potentials occur spontaneously in Acetabularia, they are therefore suggested to have a significant function for the K⁺ balance of this alga.     

Some electrophysiological and permeability properties of the mouse egg

Certain electrophysiological and ionic properties of the mouse egg (CF-1 and BDF 12–18 hr post ovulation) have been investigated. Membrane potential (?14 ± 0.4 mV, ± SE, inside negative), membrane resistance (2610 ± 38 ohm·cm²), and membrane capacitance (1.6 ± 0.03 μF cm^?2) have been determined by means of intracellular microelectrode recording techniques. Membrane potential and related parameters are stable for extended periods of time upon impalement and the magnitude of the cell membrane potential has been demonstrated to be sensitive to alteration in external sodium. The electrophysiological studies in conjunction with measurements of unidirectional potassium fluxes using isotope tracer-techniques have allowed determination of membrane permeability to potassium (8 × 10^?8 cm sec^?1) and membrane potassium conductance (25 μmho cm^?2). Furthermore, the use of tracer flux techniques has indicated that the exchangeable fraction of intracellular potassium is 204 ± 14 mM. This represents the bulk of egg potassium (222 ± 19 mM as determined from flame photometry). Studies of unidirectional potassium efflux have indicated that its movement out of the egg is made up of at least two components; an external potassium-independent potassium efflux and external potassium-dependent efflux, the latter possibly representing a potassium exchange mechanism. The combined electrophysiological and tracer-flux data indicate that only a small portion of the total membrane conductance is composed of potassium conductance at this stage of development. This and the fact that the membrane potential is far from the potassium equilibrium potential are similar to observations made on mature eggs of several other species.     

Potassium Channels in Eremosphaera viridis: Modulation of Channel Opening,Conductance and Inhibition*

I/V relationships were performed by the voltage clamp technique in the sphaerical green alga Eremosphaera viridis de Bary. We focused on the course of the transient potential (TP) found in light-off experiments when specific potassium channels open. I/V measurements done during this period show a N-shaped curve. The shape depended on external potassium. TPs could be released by light-off and by addition of barium, strontium, or α-naphthyl phosphate. We calculated the number of specific potassium channels to be between 1750 and 34 825 channels per cell. Barium (1 mol × m^?3) and tetraethylammonium (10 mol × m^?3) inhibited TPs. I/V relationships demonstrated, when N-shaped, that potassium channels start to close at voltages more negative than ?195 mV (0.1 mol × m^?3 K⁺), ?160 mV (1 mol × m^?3 K⁺) and ?148 mV (10 mol × m^?3 K⁺). In the region of ?300 mV conditions similar to those at rest are reached. External sodium suppressed the development of N-shaped I/V relationships and reduced the membrane conductance during a TP between 8 % and 29 %. This indicates an influence of external sodium on potassium channels.     

Interactions of cardiac glycosides with cultured cardiac cells: II. Biochemical and electron microscopic studies on the effects of ouabain on muscle and non-muscle cells

Electron microscopic and biochemical studies revealed a salient difference in the response to toxic doses of ouabain by cultured cardiac muscle and non-muscle cells from neonatal rats. Progressive cellular injury in myocytes incubated with 1 · 10^?4–1 · 10^?3 M ouabain ultimately leads to swelling and necrosis. The morphological damage in myocytes was accompanied by a drastic decrease in ¹⁴CO₂ formation from ¹⁴C-labeled stearate or acetate but not glucose. Neither morphological nor biochemical impairments were observed in non-muscle cells. The interaction between ouabain and the cultured cells, using therapeutic doses of ouabain (i.e., <1 · 10^?7 M), was characterized. Two binding sites were described in both classes of cells, one site is a saturable K⁺-sensitive site whereas the other is non-saturable and K⁺-insensitive. The complexes formed between the sarcolemma receptor(s) and ouabain, at low concentrations of the drug (e.g., 7.52 · 10^?9 M), had K_d values of 8.9 · 10^?8 and 2.3 · 10^?8 M for muscle and non-muscle cells, respectively. The formation and dissociation of the complexes were affected by temperature and potassium ions.     

Valinomycin inhibition of insulin release and alteration of the electrical properties of pancreatic B cells

The effects of valinomycin on insulin release and rubidium efflux from perifused isolated rat islets were investigated and correlated with its effects on the electrical properties of mouse B cells studied with microelectrode techniques. Valinomycin produced a (1 · 10^?9–1 · 10^?6 M) dose- and time-dependent inhibition of (10–15 mM) glucose-stimulated insulin release but did not affect basal secretion. This inhibitory effect rapidly followed addition of the ionophore and equally affected the two phases of glucose-stimulated secretion. It was not reversible by simple washing of the islets, but could be reversed transiently by tetraethylammonium or high extracellular potassium ion levels. At low or high glucose, valinomycin rapidly augmented the rate of ⁸⁶Rb⁺ efflux from preloaded islets. Amplitude and rapidity of this effect were dose-dependent and it was antagonized by tetraethylammonium. Glucose metabolism by islet cells was reduced only slightly (15%) by 1 · 10^?7 M valinomycin. During the first 6 to 8 min of valinomycin addition, the membrane potential of B cells augmented slowly but the typical bursts of spikes disappeared rapidly. Later on, B cells hyperpolarized more quickly to a stable value of approx. ?70 mV. Increasing extracellular K⁺ immediately depolarized B cells and the linear relationship found between the logarithm of K⁺ concentration and the membrane potential was characterized by a slope of 58 mV for a ten-fold increase in extracellular K⁺.These results suggest that valinomycin interferes with the insulin releasing effect of glucose by increasing the potassium permeability of the B cell membrane.     

An electrogenic NA+/K+ pump in the choroid plexus.

Intracellular electrical potential and potassium activity was measured by means of microelectrodes in the epithelial cells of choroid plexus from bullfrogs (Rana catesbeiana). Ouabain applied from the ventricular side caused an abrupt depolarisation of 10 mV but only a gradual loss of potassium from the cells. Readministration of potassium to the ventricular solution of plexuses which were previously depleted of potassium, caused a hyperpolarisation of about 4 mV. These two experiments are consistent with the notion of an electrogenic Na+/K+ pump situated at the ventricular membrane and which pumps potassium into the cell and sodium into the ventricle. The numerical values obtained suggest that 3 sodium ions are pumped for 2 potassium ions. The permeability coefficient for potassium exit from the cell is calculated to be 1.24 . 10(-5) cm-1 . s-1 expressed per cm2 of flat epithelium.     

On the Concept of Resting Potential—Pumping Ratio of the Na+/K+ Pump and Concentration Ratios of Potassium Ions Outside and Inside the Cell to Sodium Ions Inside and Outside the Cell

In animal cells, the resting potential is established by the concentration gradients of sodium and potassium ions and the different permeabilities of the cell membrane to them. The large concentration gradients of sodium and potassium ions are maintained by the Na⁺/K⁺ pump. Under physiological conditions, the pump transports three sodium ions out of and two potassium ions into the cell per ATP hydrolyzed. However, unlike other primary or secondary active transporters, the Na⁺/K⁺ pump does not work at the equilibrium state, so the pumping ratio is not a thermodynamic property of the pump. In this article, I propose a dipole-charging model of the Na⁺/K⁺ pump to prove that the three Na⁺ to two K⁺ pumping ratio of the Na⁺/K⁺ pump is determined by the ratio of the ionic mobilities of potassium to sodium ions, which is to ensure the time constant τ and the τ-dependent processes, such as the normal working state of the Na⁺/K⁺ pump and the propagation of an action potential. Further, the concentration ratios of potassium ions outside and inside the cell to sodium ions inside and outside the cell are 0.3027 and 0.9788, respectively, and the sum of the potassium and sodium equilibrium potentials is ?30.3 mV. A comparative study on these constants is made for some marine, freshwater and terrestrial animals. These findings suggest that the pumping ratio of the Na⁺/K⁺ pump and the ion concentration ratios play a role in the evolution of animal cells.     

Membrane potential of the unfertilized sea urchin egg

The membrane potential, specific resistance, and potassium selectivity of the unfertilized Strongylocentrotus purpuratus egg were determined by two independent methods: tracer flux and microelectrode. The potassium influx was 0.50 ± 0.2 pmole/cm²· sec, which was greater than the sodium, chloride, and calcium influxes by factors of 4, 7, and 75, respectively. By means of the constant-field equations, the flux data were used to calculate membrane potential (?70 mV) and specific resistance (420 kΩ · cm²). The effect of the external potassium concentration on the sodium influx was determined and the results closely fit the result expected if the membrane behaved as a potassium electrode. Microelectrode measurements of the potential and resistance were ?75 ± 3 mV and 380 ± kΩ · cm².     

Cell dualism: presence of cells with alternative membrane potentials in growing populations of bacteria and yeasts

It is considered that all growing cells, for exception of acidophilic bacteria, have negatively charged inside cytoplasmic membrane (Δψ^? - cells). Here we show that growing populations of microbial cells contain a small portion of cells with positively charged inside cytoplasmic membrane (Δψ⁺ - cells). These cells were detected after simultaneous application of the fluorescent probes for positive membrane potential (anionic dye DIBAC^-) and membrane integrity (propidium iodide, PI). We found in exponentially growing cell populations of Escherichia coli and Saccharomyces cerevisiae that the content of live Δψ^- - cells was 93.6?±?1.8 % for bacteria and 90.4?±?4.0 % for yeasts and the content of live Δψ⁺ - cells was 0.9?±?0.3 % for bacteria and 2.4?±?0.7 % for yeasts. Hypothetically, existence of Δψ⁺ - cells could be due to short-term, about 1 min for bacteria and 5 min for yeasts, change of membrane potential from negative to positive value during the cell cycle. This change has been shown by the reversions of K⁺, Na⁺, and Ca²⁺ ions fluxes across the cell membrane during synchronous yeast culture. The transformation of Δψ^-- cells to Δψ⁺ - cells can be explained by slow influx of K⁺ ions into Δψ^-- cell to the trigger level of K⁺ concentration (“compression of potassium spring”), which is forming “alternative” Δψ⁺-cell for a short period, following with fast efflux of K⁺ ions out of Δψ⁺-cell (“release of potassium spring”) returning cell to normal Δψ^- state. We anticipate our results to be a starting point to reveal the biological role of cell dualism in form of Δψ^- - and Δψ⁺ - cells.     

An electrophysiological study of the membrane properties of the immature and mature oocyte of the Batstar,Patiria miniata

Immature oocyte membrane properties of a starfish, Patiria miniata, were investigated by microelectrode techniques. The resting membrane potential in artificial seawater (ASW) was ?78.5 ± 6.7 mV (n = 61, inside negative). This was mainly accounted for by a selective permeability to potassium ions. Potassium ion-selective microelectrodes were used to measure intracellular K⁺ ion activity, which was 350 mM. The sodium to potassium permeability ratio was 0.02 ± 0.01 (n = 4). The current-voltage relation was nonlinear. The I–V curve included both areas of inward and outward rectification. The dependence of inward rectification upon the K⁺ ion electrochemical gradient was demonstrated. The membrane was capable of a regenerative action potential due to permeability changes for Ca²⁺ and Na⁺ ions. The Ca and Na components of the action potential were identified. The Ca component was reversibly suppressed by cobalt and irreversibly blocked by D-600. The Na component was tetrodotoxin (TTX) insensitive. The excitable response of P. miniata oocytes is similar to that described by Miyazaki et al. (1975a) for those of the starfish Asterina pectinifera.Immature oocytes were stimulated to mature with 10^?5M 1-methyladenine (1-MA) during continuous monitoring of the membrane potential. The resting potential in ASW became more inside negative during maturation. This change of the passive membrane property of the oocyte may be accounted for by the increased selectivity to K⁺ ions. The specific membrane resistance near the resting potential increased from 4.2 ± 1.4 to 21 ± 8.7 kΩ·cm² (n = 15) during maturation, while the specific membrane capacitance decreased slightly from 2 ± 0.5 to 1.7 ± 0.6 μF/cm² (n = 5). Maturation had little effect upon the active membrane properties.     

Some features of hydrogen (ion) secretion by the frog skin

We have studied the movements of H⁺ from the in vitro frog skin into the outside solution because it has been suggested that the movement of sodium from the outside solution into the skin may result from the forced exchange of Na⁺ by H⁺.Our main observations can be summarized as follows: (a) Hydrogen moves from the skin into the outside solution at a rate of 0.04 μequiv · cm^?2 · h^?1 while Na⁺ influx had a value of 0.49 μequiv · cm^?2 · h^?1. (b) The rate of H⁺ secretion is not significantly affected by substituting the Na⁺ in the outside solution by K⁺ nor by inhibiting Na⁺ influx with amiloride (5 · 10^?5 M). (c) Acetazolamide (5 · 10^?3 M) blocked H⁺ secretion without altering the potential difference across the skin. (d) The rate of H⁺ production is not underestimated because it may have been neutralized by HCO₃^? secreted into the outside solution in exchange for Cl^?. Substituting all the Cl^? by SO₄^2? in the outside solutions does not result in an increase in the rate of H⁺ production. (e) The steady-state rate of H⁺ secretion is not affected by large changes in electrochemical potential gradients for H⁺. Neither abolishing the potential difference across the skin nor a 10-fold change in H⁺ concentration in the outside solution affected significantly the steady-state rate of H⁺ secretion. (f) The H⁺ secretion was abolished by the metabolic inhibitors dinitrophenol (1 · 10^?4 M) and Antimycin A (1.5 · 10^?6 M) which also markedly reduced the potential difference across the skin.Observations (a), (b), and (c) suggest that H⁺ and Na⁺ movements across the outer border of the isolated frog skin are not coupled. The ratio of Na⁺ to H⁺ movements is very different from unity and Na⁺ movements can be abolished without any effects on H⁺ secretion and conversely H⁺ movements can be abolished without interruption of Na⁺ uptake.A second conclusion suggested by these results is that the H⁺ secretion does not result from movement of H⁺ following its electrochemical potential gradient since that rate of secretion is not affected by marked changes in either potential or [H⁺]. Furthermore, the effects of metabolic inhibitors suggest that H⁺ secretion requires the expenditure of energy by the cell.     

A study of the current-voltage relationships of electrogenetic active and passive membrane elements in riccia fluitans

Potassium- and proton-dependent membrane potential, conductance, and current-voltage characteristics (I–V curves) have been measured on rhizoid cells of the liverwort Riccia fluitans. The potential difference (E_m) measured with microelectrodes across plasmalemma and tonoplast is depolarized to the potassium-sensitive diffusion potential (E_D) in the presence of 1 mM NaCN, 1 mM NaN₃, or at temperatures below 6°C. Whereas the temperature change from 25°C to 5°C decreases the membrane conductance (g_m) from 0.71 to 0.43 S ? m^?2, 1 mM NaCN increases g_m by about 25%. The membrane displays potassium-controlled rectification which gradually disappears at temperatures below 5°C. The potassium pathway can be described by an equivalent circuit of a diode and an ohmic resistor in parallel. In the potential interval of E_D ± 100 mV the measured I-V curves roughly fit the theoretical curves obtained from a modified diode equation. ⁸⁶Rb⁺(K⁺)-influx is voltage sensitive: In the presence of 1 mM NaCN, ⁸⁶Rb⁺-influx follows a hyperbolic function corresponding to a low conductance at low [K⁺]_o and high conductance at high [K⁺]_o. On the contrary ⁸⁶Rb⁺-influx is linear with [K⁺]_o when pump activity is normal. It is believed that there are two K⁺-transport pathways in the Riccia membrane, one of which is assigned to the low conductance (0.2 S · m^?2), the other to a temperature-dependent facilitated diffusion system with a higher conductance (7.7 S · m^?2). The electrogenic pump essentially acts as a current source and consumes about 39% of the cellular ATP-turnover. In the presence of 30 μM CCCP the saturation current of 0.1 A · m^?2 is doubled to about 0.2 A · m^?2, and the electromotive force of ?360 mV switches to ?250 mV. It is suggested that this may be due to a change in stoichiometry from one to two transported charges per ATP hydrolyzed.     

Electrokinetic properties of asparaginase sensitive or resistant mouse leukemic cells treated with L-asparaginase

The electrophoretic mobility of L5178Y cells in 0.0145 M NaCl, 4.5% sorbitol, 0.6 mM NaHCO₃, pH 7.2, at 25°C was — 1.78 μ·s^?1·V^?1·cm^?1 while that of an L-asparaginase resistant subline, L5178Y/ASN, was — 1.11 μm·s^?1·V^?1·cm^?1. Both cell lines were characterized by terminal sialic acid residues on their surfaces. Treatment of L5178Y cells for 90 min with 10 units of L-asparaginase per ml in saline decreased the electrophoretic mobility of the cells to — 1.65 μm·s^?1·V^?1·cm^?1 while treatment in Fischer's medium decreased the mobility to — 1.25 μm·s^?1·V^?1·cm^?1; neither treatment had a significant effect on the L5178Y/ASN electrophoretic mobility. The results suggest that L-asparaginase has an immediate and specific effect on synthesis of cell surface asparaginyl glycoproteins.     

Maturation and fertilization of the sea urchin oocyte: An electrophysiological study

Some electrical properties of the sea urchin oocyte during germinal vesicle breakdown (GVBD) and fertilization have been studied using two intracellular electrodes. Oocytes with distinct germinal vesicles have resting potentials of ?70 to ?90 mV and the specific membrane resistance may range from 3 to 10 kΩ·cm². Around rest the I–V relationship is concave toward the axis origin and the membrane is K⁺ selective. A second electrical state, of lower potential and higher resistance, preexists in the membrane. Following GVBD, the K⁺-selective system is lost and the oocyte attains the characteristics of the second state with a resting potential of ?10 to ?50 mV and specific membrane resistance of 10–50 kΩ·cm². At rest the I–V relationship tends to be convex toward the axis origin. The majority of sea urchin eggs (which have undergone GVBD and completed meiosis) have a resting state of ?10 to ?30 mV; 10–50 kΩ·cm². The I–V relationship around rest is convex toward the axis origin and the resting potential is sensitive to changes of Na⁺, Cl^?, and K⁺ in the external medium. There is probably no major change in the electrical properties of the oocyte during the completion of meiosis. A small percentage of eggs from suboptimal animals have high resting potentials of ?70 to ?90 mV and specific membrane resistance of 5–50 kΩ·cm². Such eggs have predominantly K⁺-selective membranes and we suggest that they are either underripe or aged. The first electrical event across the egg plasma membrane during fertilization is a step-like depolarization which occurs about 2 sec after the attachment of the fertilizing spermatozoon to the vitelline layer. There is no change—at the level of the light microscope—either in the egg surface or in the behavior of the spermatozoon until the second event, the fertilization potential (FP), is initiated 11 sec later. The cortical reaction occurs simultaneously with the FP and during the rising phase of the FP the spermatozoon stops gyrating around its point of attachment. Oocytes, which do not have cortical granules, upon insemination exhibit step events but no FP; in contrast artificially activated eggs, either spontaneous or induced by the ionophore A23187, give rise to only the FP. We suggest that the FP is the electrical result of the modification of the egg plasma membrane during cortical exocytosis.     

The kinetics of sodium extrusion in striated muscle as functions of the external sodium and potassium ion concentrations

After a 20 min initial washout, the rate of loss of radioactively labeled sodium ions from sodium-enriched muscle cells is sensitive to the external sodium and potassium ion concentrations. In the absence of external potassium ions, the presence of external sodium ions increases the sodium efflux. In the presence of external potassium ions, the presence of external sodium ions decreases the sodium efflux. In the absence of external potassium ions about one-third of the Na⁺ efflux that depends upon the external sodium ion concentration can be abolished by 10^-5 M glycoside. The glycoside-insensitive but external sodium-dependent Na⁺ efflux is uninfluenced by external potassium ions. In the absence of both external sodium and potassium ions the sodium efflux is relatively insensitive to the presence of 10^-5 M glycoside. The maximal external sodium-dependent sodium efflux in the absence of external potassium ions is about 20% of the magnitude of the maximal potassium-dependent sodium efflux. The magnitude of the glycoside-sensitive sodium efflux in K-free Ringer solution is less than 10% of that observed when sodium efflux is maximally activated by potassium ions. The inhibition of the potassium-activated sodium efflux by external sodium ions is of the competitive type. Reducing the external sodium ion concentration displaces the plots of sodium extrusion rate vs. [K]_o to the left and upwards.     

Interaction of dichlone with human erythrocytes. I. Changes in cell permeability

The uptake of the fungicide dichlone (2,3-dichloro-1,4-naphthoquinone) by human erythrocytes was extremely rapid, reaching a maximum within 5 min of treatment. Most of the dichlone taken up was present in the interior of the cell; only a small fraction of the pesticide (less than 5%) was bound to the cell membrane. Dichlone (3 · 10^?5M-10^?4M) induced a rapid loss of intracellular potassium from the erythrocytes; the leakage of K⁺ varied with the fungicide concentration as well as with cell concentration. Pretreatment of the cells with glutathione was able to reduce potassium loss. Cells exposed to dichlone showed increased osmotic fragility. Dichlone also inhibited Na⁺-K⁺ ATPase, which is associated with active ion transport. However, the leakage of potassium in dichlone-treated cells does not appear to be related to the interference with active ion transport. An extensive loss of potassium within a relatively short time after treatment suggests that dichlone produces its effect by increasing passive cation permeability, probably as a result of direct action on the membrane structure. Dichlone was able to induce hemolysis, but only at concentrations higher than those which resulted in K⁺ loss. The loss of hemoglobin appeared to be mainly due to osmotic swelling of the treated cells. Exposure of red cells to dichlone also resulted in a rapid and extensive formation of methemoglobin as well as a denaturation of hemoglobin. Thus, dichlone not only may be capable of lowering the capacity of erythrocytes to transport oxygen but also alters their permeability.     

Characterization of sodium and proton flows in sub-bacterial particles of Halobacterium halobium in terms of nonequilibrium thermodynamics

A thermodynamic characterization of the Na⁺-H⁺ exchange system in Halobacterium halobium was carried out by evaluating the relevant phenomenological parameters derived from potential-jump measurements. The experiments were performed with sub-bacterial particles devoid of the purple membrane, in 1 M NaCl, 2 M KCl, and at pH 6.5–7.0. Jumps in either pH or pNa were brought about in the external medium, at zero electric potential difference across the membrane, and the resulting relaxation kinetics of protons and sodium flows were measured. It was found that the relaxation kinetics of the proton flow caused by a pH-jump follow a single exponential decay, and that the relaxation kinetics of both the proton and the sodium flows caused by a pNa-jump also follow single exponential decay patterns. In addition, it was found that the decay constants for the proton flow caused by a pH-jump and a pNa-jump have the same numerical value. The physical meaning of the decay constants has been elucidated in terms of the phenomenological coefficients (mobilities) and the buffering capacities of the system. The phenomenological coefficients for the Na⁺-H⁺ flows were determined as differential quantities. The value obtained for the total proton permeability through the particle membrane via all available channels, $\text{L}{}_{\mathrm{<mtext>H</mtext>}}\text{= (}\text{?J}{}_{\mathrm{<mtext>H\; +</mtext>}}\text{?Δ}\text{pH}\text{)}{}_{\mathrm{<mtext>\Delta \psi ,\Delta </mtext><mtext>pNa</mtext>}}$, was in the range of 850–1150 nmol H⁺·(mg protein)^?1·h^?1·(pH unit)^?1 for four different preparations; for the total Na⁺ permeability, $\text{L}{}_{\mathrm{<mtext>Na</mtext>}}\text{= (}\text{?J}{}_{\mathrm{<mtext>Na</mtext>}}{}^{\mathrm{+}}\text{?Δ}\text{pNa}\text{)}{}_{\mathrm{<mtext>\Delta \psi ,\Delta </mtext><mtext>pH</mtext>}}$, it was 1620–2500 nmol Na⁺·(mg protein)^?1·h^?1·(pNa unit)^?1; and for the proton ‘cross-permeability’, $\text{L}{}_{\mathrm{<mtext>HNa</mtext>}}\text{= (}\text{?J}{}_{\mathrm{<mtext>H</mtext>}}{}^{\mathrm{+}}\text{?Δ}\text{pNa}\text{)}{}_{\mathrm{<mtext>\Delta \psi ,\Delta </mtext><mtext>pH</mtext>}}$, it was 220–580 nmol H⁺·(mg protein)^?1·h^?1·(pNa unit)^?1, for different preparations. From the above phenomenological parameters, the following quantities have been calculated: the degree of coupling (q), the maximal efficiency of Na⁺-H⁺ exchange (η_max), the flow and force efficacies (?) of the above exchange, and the admissible range for the values of the molecular stoichiometry parameter (r). We found q ? 0.4; η_max ? 5%; 0.36 ? r ? 2; ?_JNa⁺ ? 1.3 · 10⁵μmol · (RT unit)^?1 at J_Na = 1 μmolNa⁺ · (mgprotein)^?1 · h^?1; and ?_ΔpNa ? 5 · 10⁴ ΔpNa · (mg protein) · h · (RT unit)^?1 at ΔpNa = 1 unit, for different preparations.     

Possible epithelial sodium channels visualized by freeze-fracture

The coprodeum is a very efficient Na⁺-retaining epithelium. Coprodeum from birds on a high Na⁺ diet has virtually no ion transport, while an Amiloride-sensitive Na⁺ absorption of 10–12 μ equiv·cm^?2·h^?1 is induced in the coprodeal epithelium from birds on a low Na⁺ diet. Both measurements of the Na⁺ influx and Na⁺-diffusion potentials across the luminal cell membrane have revealed a selective opening of this membrane to Na⁺ in birds on a low Na⁺ diet. Freeze-fracture P faces of the luminal membrane in coprodea taken from birds on a low Na⁺ diet have rod-shaped particles, $\text{100 × 240}\text{A}\text{?}$, in more than 20% of the principal cells. Rod-shaped particles appear in less than 1% of these cells in coprodea from high Na⁺-diet birds. Thus a low Na⁺ diet induces rod-shaped particles in the luminal cell membrane of the hen coprodeum. These new particles may function as Na⁺-channels mediating the increased Na⁺-influx across the apical cell membrane.     

Voltage-sensitive chloride ion channels in Anopheles gambiae Sua-1B cells

In this study, we performed electrophysiological analysis of Anopheles gambiae Sua-1B cells having “neuron-like” morphologies using the patch clamp method. The recorded cells (n = 79) had processes resembling axons/dendrites, with 63 % unipolar, 22 % bipolar, and 15 % multipolar. While no inward currents were observed following step depolarizations (holding potential = ?80 mV), a slowly activating outward current was observed in 96 % of the cells, especially at depolarized potentials. The amplitude of the current was attenuated nearly 70 % by reducing extracellular Cl^? ion concentration, or by incubating with 100 μM DIDS, a known voltage-sensitive chloride channel blocker, suggesting that the current was mediated by chloride ions. No qualitative difference was found between recordings made with Cs⁺ ions in the intracellular pipette solution (inhibits K⁺ currents) and those made with normal physiological solution, indicating a deficiency of potassium channels. Additionally, recordings made with Ca²⁺-free extracellular bath solution eliminated the slowly activating outward current. A subset of cells (n = 3) lacked this current, but had outward currents with voltage-dependent properties similar to those of volume-regulated chloride channels. Taken together, our results suggest that the voltage-sensitive currents observed in the majority of Sua-1B cells are mediated primarily by chloride channels of the calcium-dependent subtype.