Intracellular Na+, K+, and C1- activities in Balanus photoreceptors

Ion-sensitive microelectrodes were used to measure intracellular activities (aix) of Na+, K+, and C-1 in Balanus photoreceptors. Average values of aiNa, aiK, and aiCl were 28 mM, 120 mM, and 65 mM, respectively. Equilibrium potentials calculated from these average values were: Na+ +64 mV, K+ - 77 mV, and and Cl- -42 mV; ther average value of the resting potential for all cells examined was -41 mV. Long exposure to intense illumination produced measurable increases in aiNa. Classical Na+ - K+ reciprocal dilution experiments were analyzed with and without observed changes in aiK. As aoK was increased, the membrane depolarized, and aiK increased. Better agreement was found between the membrane potential and the directly determined EK than expected from the standard relation between Em and aoK. The latter produced pNa:pK estimates of the resting photoreceptor membrane that were higher than estimates based on data from the ion electrodes. Generally, Em was more negative than EK as aoK was increased. This is consistent with a significant chloride permeability in the dark-adapted photoreceptor.     

Intrinsic gating of inward rectifier in bovine pulmonary artery endothelial cells in the presence or absence of internal Mg2+

Inward rectifier (IR) currents were studied in bovine pulmonary artery endothelial cells in the whole-cell configuration of the patch-clamp technique with extracellular K+ concentrations, [K+]o, ranging from 4.5 to 160 mM. Whether the concentration of free Mg2+ in the intracellular solution, [Mg2+]i, was 1.9 mM or nominally 0, the IR exhibited voltage- and time-dependent gating. The IR conductance was activated by hyperpolarization and deactivated by depolarization. Small steady-state outward IR currents were present up to approximately 40 mV more positive than the K+ reversal potential, EK, regardless of [Mg2+]i. Modeled as a first-order C in equilibrium O gating process, both the opening rate, alpha, and the closing rate, beta, were exponentially dependent on voltage, with beta more steeply voltage dependent, changing e-fold for 9 mV compared with 18 mV for an e-fold change in alpha. Over all [K+]o studied, the voltage dependence of alpha and beta shifted along with EK, as is characteristic of IR channels in other cells. The steady-state voltage dependence of the gating process was well described by a Boltzmann function. The half-activation potential was on average approximately 7 mV negative to the observed reversal potential in all [K+]o regardless of [Mg2+]i. The activation curve was somewhat steeper when Mg-free pipette solutions were used (slope factor, 4.3 mV) than when pipettes contained 1.9 mM Mg2+ (5.2 mV). The simplest interpretation of these data is that IR channels in bovine pulmonary artery endothelial cells have an intrinsic gating mechanism that is not due to Mg block.     

Inhibition of endothelium-dependent vasorelaxation by extracellular K(+): a novel controlling signal for vascular contractility

The effects of extracellular K+ on endothelium-dependent relaxation (EDR) and on intracellular Ca2+ concentration ([Ca2+]i) were examined in mouse aorta, mouse aorta endothelial cells (MAEC), and human umbilical vein endothelial cells (HUVEC). In mouse aortic rings precontracted with prostaglandin F2alpha or norepinephrine, an increase in extracellular K+ concentration ([K+]o) from 6 to 12 mM inhibited EDR concentration dependently. In endothelial cells, an increase in [K+]o inhibited the agonist-induced [Ca2+]i increase concentration dependently. Similar to K+, Cs+ also inhibited EDR and the increase in [Ca2+]i concentration dependently. In current-clamped HUVEC, increasing [K+]o from 6 to 12 mM depolarized membrane potential from -32.8 +/- 2.7 to -8.6 +/- 4.9 mV (n = 8). In voltage-clamped HUVEC, depolarizing the holding potential from -50 to -25 mV decreased [Ca2+]i significantly from 0.95 +/- 0.03 to 0.88 +/- 0.03 microM (n = 11, P < 0.01) and further decreased [Ca2+]i to 0.47 +/- 0.04 microM by depolarizing the holding potential from -25 to 0 mV (n = 11, P < 0.001). Tetraethylammonium (1 mM) inhibited EDR and the ATP-induced [Ca2+]i increase in voltage-clamped MAEC. The intermediate-conductance Ca2+-activated K+ channel openers 1-ethyl-2-benzimidazolinone, chlorozoxazone, and zoxazolamine reversed the K+-induced inhibition of EDR and increase in [Ca2+]i. The K+-induced inhibition of EDR and increase in [Ca2+]i was abolished by the Na+-K+ pump inhibitor ouabain (10 microM). These results indicate that an increase of [K+]o in the physiological range (6-12 mM) inhibits [Ca2+]i increase in endothelial cells and diminishes EDR by depolarizing the membrane potential, decreasing K+ efflux, and activating the Na+-K+ pump, thereby modulating the release of endothelium-derived vasoactive factors from endothelial cells and vasomotor tone.     

Electrochemical potentials of potassium in skeletal muscle under different metabolic states.

Intracellular potassium and membrane potential were measured simultaneously by means of double-barrelled liquid ion-exchange microelectrodes in single fibers of rat thigh muscle in vivo in rats maintained in seven different metabolic states. The K+ equilibrium potential (EK) was more negative than the simultaneously measured membrane potential (Em) in the normal state by 18.4 mV. K+ loading, acute and chronic, resulted in depolarization of Em due to increased serum K+ (hyperkalemia) with no increase in intracellular K+. K+ depletion resulted in hyperpolarization of Em as plasma K+ decreased proportionately more than intracellular K+. Low Na+ diet had no effect. Intracellular K+ was decreased in acute acidosis but not in the chronic state. Thus K+ depletion and acute acidosis are associated with intracellular K+ decrease. The fact that hyperpolarization exists in the former and not the latter is a reflection that hypokalemia accompanies the former condition. The hyperpolarizing states of K+ depletion and chronic acidosis are accompanied by decreased excitability and muscle weakness.     

Effects of intracellular and extracellular concentrations of Ca2+, K+, and Cl- on the Na+-dependent Mg2+ efflux in rat ventricular myocytes

Intracellular Mg2+ concentration ([Mg2+]i) was measured in rat ventricular myocytes with the fluorescent indicator furaptra (25 degrees C). After the myocytes were loaded with Mg2+, the initial rate of decrease in [Mg2+]i (initial Delta[Mg2+]i/Deltat) was estimated upon introduction of extracellular Na+, as an index of the rate of Na+-dependent Mg2+ efflux. The initial Delta[Mg2+]i/Deltat values with 140 mM [Na+]o were essentially unchanged by the addition of extracellular Ca2+ up to 1 mM (107.3+/-8.7% of the control value measured at 0 mM [Ca2+]o in the presence of 0.1 mM EGTA, n=5). Intracellular loading of a Ca2+ chelator, either BAPTA or dimethyl BAPTA, by incubation with its acetoxymethyl ester form (5 microM for 3.5 h) did not significantly change the initial Delta[Mg2+]i/Deltat: 115.2+/-7.5% (seven BAPTA-loaded cells) and 109.5+/-10.9% (four dimethyl BAPTA loaded cells) of the control values measured in the absence of an intracellular chelator. Extracellular and/or intracellular concentrations of K+ and Cl- were modified under constant [Na+]o (70 mM), [Ca2+]o (0 mM with 0.1 mM EGTA), and membrane potential (-13 mV with the amphotericin-B-perforated patch-clamp technique). None of the following conditions significantly changed the initial Delta[Mg2+]i/Deltat: 1), changes in [K+]o between 0 mM and 75 mM (65.6+/-5.0% (n=11) and 79.0+/-6.0% (n=8), respectively, of the control values measured at 140 mM [Na+]o without any modification of extracellular and intracellular K+ and Cl-); 2), intracellular perfusion with K+-free (Cs+-substituted) solution from the patch pipette in combination with removal of extracellular K+ (77.7+/-8.2%, n=8); and 3), extracellular and intracellular perfusion with K+-free and Cl--free solutions (71.6+/-5.1%, n=5). These results suggest that Mg2+ is transported in exchange with Na+, but not with Ca2+, K+, or Cl-, in cardiac myocytes.     

Binding of S-adenosylhomocysteine to hydroxyindole O-methyltransferase

Mg2+-selective microelectrodes have been used to measure the intracellular free Mg2+ concentration in frog skeletal muscle fibers. Glass capillaries with a tip diameter of less than 0.4 micron were backfilled with the Mg2+ sensor, ETH 1117. In the absence of interfering ions, they gave Nernstian responses between 1 and 10 mM free Mg2+. In the presence of an ionic environment resembling the myoplasm, the microelectrode response was sub Nernstian (18-24 mV) but still useful. The electrodes were calibrated before and after muscle-fiber impalements . In quiescent fibers from sartorius muscle (Rana pipiens), with resting membrane potentials not less than -82 mV, the intracellular free Mg2+ concentration was 3.8 +/- 0.41 (S.E.) mM (n = 58) at 22 degrees C. No significant change in the intracellular free Mg2+ was observed following extensive (approx. 6 h) incubation in Mg2+-free media. Increasing the external concentration of magnesium from 4 to 20 mM (approx. 15 min) produced a slow and small enhancement (1.8 mM) of [Mg2+]i, which was fully reverted when the divalent cation was removed from the bathing solution. No change in ionic magnesium resting concentration was observed when the muscle fibers were treated either with caffeine 3 mM or with Na+-free solutions. In depolarized muscle fibers (-23 +/- 2.7 mV) treated with 100 mM K+, the myoplasmic [Mg2+] was 3.7 +/- 0.45 (S.E.) mM, n = 6, immediately after the spontaneous relaxation of the contracture. Similar determinations in muscle fibers during stimulation at low frequency (5 Hz), and after fatigue development, showed no changes in the concentration of free cytosolic Mg2+. These results point out that [Mg2+]i is not modified under these three different experimental conditions.     

The pacemaker current in cardiac Purkinje myocytes

It is generally assumed that in cardiac Purkinje fibers the hyperpolarization activated inward current i(f) underlies the pacemaker potential. Because some findings are at odds with this interpretation, we used the whole cell patch clamp method to study the currents in the voltage range of diastolic depolarization in single canine Purkinje myocytes, a preparation where many confounding limitations can be avoided. In Tyrode solution ([K+]o = 5.4 mM), hyperpolarizing steps from Vh = -50 mV resulted in a time-dependent inwardly increasing current in the voltage range of diastolic depolarization. This time- dependent current (iKdd) appeared around -60 mV and reversed near EK. Small superimposed hyperpolarizing steps (5 mV) applied during the voltage clamp step showed that the slope conductance decreases during the development of this time-dependent current. Decreasing [K+]o from 5.4 to 2.7 mM shifted the reversal potential to a more negative value, near the corresponding EK. Increasing [K+]o to 10.8 mM almost abolished iKdd. Cs+ (2 mM) markedly reduced or blocked the time-dependent current at potentials positive and negative to EK. Ba2+ (4 mM) abolished the time-dependent current in its usual range of potentials and unmasked another time-dependent current (presumably i(f)) with a threshold of approximately -90 mV (> 20 mV negative to that of the time-dependent current in Tyrode solution). During more negative steps, i(f) increased in size and did not reverse. During i(f) the slope conductance measured with small (8-10 mV) superimposed clamp steps increased. High [K+]o (10.8 mM) markedly increased and Cs+ (2 mM) blocked i(f). We conclude that: (a) in the absence of Ba2+, a time-dependent current does reverse near EK and its reversal is unrelated to K+ depletion; (b) the slope conductance of that time-dependent current decreases in the absence of K+ depletion at potentials positive to EK where inactivation of iK1 is unlikely to occur. (c) Ba2+ blocks this time-dependent current and unmasks another time-dependent current (i(f)) with a more negative (> 20 mV) threshold and no reversal at more negative values; (d) Cs+ blocks both time-dependent currents recorded in the absence and presence of Ba2+. The data suggest that in the diastolic range of potentials in Purkinje myocytes there is a voltage- and time-dependent K+ current (iKdd) that can be separated from the hyperpolarization- activated inward current i(f).     

Changes in the potassium ion concentration in the extracellular space of rat cerebral cortex during the arousal reaction.

The integrative activity of K+ ions in the CNS was studied in urethane-anaesthetized rats. Changes in the potassium ion concentration in the extracellular space ([K+]e) of the cerebral cortex were studied by means of ion-selective K+ microelectrodes introduced into the brain with an implanted micro-drive allowing measurement in the immobilized animal. EEG desynchronizations evoked by various arousal stimuli or of spontaneous origin were accompanied by a small, but definitely measurable and reliably reproducible [K+]e increment. In arousal reactions evoked by nociceptive stimuli and ammonia fumes, [K+]e rose from a resting value of 3 mM by a mean 0.31 +/- 0.04 mM and 0.61 +/- 0.15 mM respectively. The mean duration of the increase was 37 and 305 sec and the mean duration of corresponding EEG desynchronization 47 and 48 sec; the amplitude of the [K+]e change lagged 15 and 39 sec behind maximum EEG desynchronization. Periodic spontaneous desynchronizations lasting 123 sec, which were evidently associated with the sleep cycle and were accompanied by a [K+]e increment of 0.4 +/- 0.04 mM, occurred in two rats. Repeated nociceptive stimuli led to the elaboration of a conditioned arousal reaction manifested in a [K+]e increment prior to their application. [K+]e changes in arousal reactions were found to be a more sensitive index of the general activity of the neuronal population than DC potential changes.     

Electrophysiological properties of frog olfactory supporting cells

Cells, identified as supporting cells by Lucifer Yellow injection, were recorded from slices of frog olfactory epithelium using patch-clamp recordings. Cell-attached single-channel recordings indicated that the intracellular potential (IP) was -68 +/- 7 mV (n = 22) with 4 mM K+ in the bath ([K+]o). IP was -67 +/- 4 mV (n = 32) in whole-cell conditions with 100 mM KCl inside the cell, suggesting a low membrane permeability for Cl-. IP depended on [K+]o in a manner described by the Goldman- Hodgkin-Katz equation with a permeability ratio pk+:PNa+ of 40. The input resistance was 32 +/- 14 M omega (n = 15), indicating a high membrane conductance at rest. Odorant stimulations evoked passive membrane depolarizations, probably reflecting an increase in [K+]o due to the neuronal activation. Whole-cell recordings with 100 mM CsCl instead of KCl in the pipette, together with the block of gap-junctions with octanol, indicated the existence of an electrical coupling between supporting cells. The electrical coupling between these glial-like cells could facilitate the clearance of K+ ions released by olfactory receptor neurons during odorant stimulation.      

Relationship between myoplasmic calcium transients and calcium currents in frog skeletal muscle

Ca2+ currents (ICa) and myoplasmic Ca2+ transients were simultaneously recorded in single muscle fibers from the semitendinosus muscle of Rana pipiens. The vaseline-gap voltage-clamp technique was used. Ca2+ transients were recorded with the metallochromic indicator dye antipyrylazo III. Ca2+ transients consisted of an early fast rising phase followed by a late slower one. The second phase was increased by experimental maneuvers that enlarged ICa, such as augmenting [Ca2+]o (from 2 to 10 mM) or adding (-)-Bay K 8644 (2 microM). When [Ca2+]o was increased, the second phase of the Ca2+ transients and ICa showed an average increase at 0 mV of 2 +/- 0.9 microM (4) and 1.4 +/- 0.3 mA/ml (4), respectively. (-)-Bay K 8644 increased the late phase of the Ca2+ transients and ICa at 0 mV by 0.8 +/- 0.3 microM (3) and 6.7 +/- 2.0 mA/ml (4), respectively. The initial fast rising phase of the Ca2+ transients was not modified. (-)-Bay K 8644 slowed the time constant of decay of the transients by 57 +/- 6 ms. In other experimental conditions, Ca2+ release from the sarcoplasmic reticulum (SR) was impaired with repetitive stimulation in 1 mM [EGTA]i-containing fibers. Under those circumstances, Ca2+ transients directly followed the time integral of ICa. Pulses to 0 mV caused a large Ca2+ transient that became suppressed when large pulses to 100 mV were applied. In fibers with functioning SR, pulses to 100 mV elicited somewhat smaller or similar amplitude Ca2+ transients when compared with those elicited by pulses to 0 mV. The increase in ICa after raising [Ca2+]o or adding (-)-Bay K 8644 cannot directly explain the change in Ca2+ transients in fibers with functioning SR. On the other hand, when Ca2+ release from the SR is impaired Ca2+ transients depend on ICa.     

Glucose-induced oscillatory changes in extracellular ionized potassium concentration in mouse islets of Langerhans.

Liquid membrane [K+]-sensitive microelectrodes (1-2 micron tip diameter) were used to measure the extracellular ionized potassium concentration in mouse pancreatic islets of Langerhans. With the tip of the microelectrode at the surface of the islet, the time course of the [K+]-sensitive electrode potential changes in response to the application of rapid changes in [K+]o (from 1.25 to 5 mM), could be reproduced by the equation for K+-diffusion through a 100-micron-thick unstirred layer around the islet (diffusion coefficient for K+ at 27 degrees C, DK,o, taken as 1.83 X 10(-5) cm2/s). The time to reach 63% of the steady-state electrode response with the tip in the chamber at the surface of the islet was from 5 to 6 s. When the tip of the [K+]-sensitive electrode was placed in the islet tissue, the time for the response to reach 63% of the steady-state level increased. The time course of the [K+]-sensitive electrode response could be reproduced using the same diffusion model assuming that K+ diffusion into the islet tissue takes place in a tortuous intercellular path with an apparent diffusion coefficient, DK,I, about half of DK,o, in series with the unstirred layer around the islet. In the absence of glucose the potassium concentration in the extracellular space, [K+]I, was found to be higher than the concentration in the external modified Krebs solution, [K+]o. The difference in concentration [K+]I - [K+]o was greater when [K+]o was smaller than 2 mM. In the presence of glucose (between 11 and 16 mM), under steady-state conditions, small oscillatory changes in the [K+], (1.48 +/- 0.94 mM) were detected. Simultaneous recording of membrane potential from one B-cell and [K+], in the same islet indicated that the potassium concentration increased during the active phase of the bursts of electrical activity. Maximum concentration in the intercellular was reached near the end of the active phase of the bursts. We propose that the space between islet cells constitutes a restricted diffusion system where potassium accumulates during the transient activation of potassium channels.     

Ca2+-activated K+ conductance of human red cell membranes exhibits two different types of voltage dependence

The voltage dependence for outward-going current of the Ca-activated K+ conductance (gK(Ca] of the human red cell membrane has been examined over a wide range of membrane potentials (Vm at constant values of [K+]ex, [K+]c and pHc, the intact cells being preloaded to different concentrations of ionized calcium. Outward-current conductances were calculated from initial net effluxes of K+ and the corresponding (Vm - EK) values. The basic conductance, defined as the outward-current conductance at (Vm - EK) greater than or equal to 20 mV and [K+]ex greater than or equal to 3 mM (B. Vestergaard-Bogind, P. Stampe and P. Christophersen, J. Membrane Biol. 95:121-130, 1987) was found to be a function of cellular ionized Ca. At all degrees of Ca activation gK(Ca) was an apparently linear function of voltage (Vm range -40 to +70 mV), the absolute level as well as the slope decreasing with decreasing activation. In a simple two-state model the constant voltage dependence can, at the different degrees of Ca activation, be accounted for by a Boltzmann-type equilibrium function with an equivalent valence of approximately 0.4, assuming chemical equilibrium at Vm = 0 mV. Alternatively, the phenomenon might be explained by a voltage-dependent block of the outward current by an intracellular ion. Superimposed upon the basic conductance is the apparently independent inward-rectifying steep voltage function with an equivalent valence of approximately 5 and chemical equilibrium at the given EK value.     

Transmembrane potential and intracellular potassium ion activity in fetal and maternal liver

We have compared transmembrane potentials (Em) of maternal liver with Em of fetal liver, and as an initial step to account for differences in Em, we have measured intracellular potassium ion activities (aiK) in both tissues. Paired segments of maternal and fetal (day 17) mouse liver were suffused (15 ml/min) with Krebs' physiologic salt solution equilibrated with 95% 02-5% CO2 (pH 7.3-7.4) at 37 degrees C. To measure Em, cells were impaled with open-tip microelectrodes filled with 0.5 M KCl. Intracellular voltage recordings that were stable +/- 2 mV for at least 10 s were considered valid impalements. Maternal liver mean Em = -41 +/- 1 (SEM) mV, n = V 10 animals. In contrast, fetal liver mean Em = -23 +/- 1 (SEM) mV, n = 10 animals. In the same segments we measured aiK with potassium-selective liquid ion-exchanger microelectrodes. Maternal liver mean aik = 95 +/- 7 (SEM) mM and fetal liver mean aiK = 62 +/- 4 (SEM) mM. in addition, Em and aiK of fetal liver increased to values comparable to those of maternal liver during the first 8 days of neonatal life. The differences of Em and aik between fetal and maternal liver, and the changes in these values that occur in the neonate, may result from activity of a membrane Na-K exchange pump that increases with tissue development.     

Effects of the rod receptor potential upon retinal extracellular potassium concentration

It has been hypothesized that the light-evoked rod hyperpolarization (the receptor potential) initiates the light-evoked decrease in extracellular potassium ion concentration, [K+]o, in the distal retina. The hypothesis was tested using the isolated, superfused retina of the toad, Bufo marinus; the receptor potential was recorded intracellularly from red rods, and [K+]o was measured in the photoreceptor layer with K+-specific microelectrodes. In support of the hypothesis, variations in stimulus irradiance or duration, or in retinal temperature, produced qualitatively similar effects on both the receptor potential and the decrease in [K+]o. A mechanism for the relationship between the receptor potential and the decrease in [K+]o was suggested by Matsuura et al. (1978. Vision Res. 18:767-775). In the dark, the passive efflux of K+ out of the rod is balanced by an equal influx of K+ fromthe Na+/K+ pump. The light-evoked rod hyperpolarization is assumed to reduce the passive efflux, with little effect on the pump. Thus, the influx will exceed the efflux, and [K+]o will decrease. Consistent with this mechanism, the largest and most rapid decrease in [K+]o was measured adjacent to the rod inner segments, where the Na+/K+ pump is most likely located; in addition, inhibition of the pump with ouabain abolished the decrease in [K]o more rapidly than the rod hyperpolarization. Based upon this mechanism, Matsuura et al. (1978) developed a mathematical model: over a wide range of stimulus irradiance, this model successfully predicts the time-course of the decrease in [K+]o, given only the time-course of the rod hyperpolarization.     

Effects of catecholamines and potassium on cardiovascular performance in the rabbit.

Resting subjects risk cardiac arrest if plasma potassium ([K+]p) is raised rapidly to 7-9 mM, but brief bouts of exhaustive exercise in healthy subjects can give similar [K+]p without causing cardiac problems. We investigated the effects of [K+]p and catecholamines on systolic blood pressure (SBP) and mean aortic flow (MAF) in anesthetized rabbits and on maximum output pressure (MOP) in isolated working rabbit hearts. In six rabbits, hyperkalemia (11.4 +/- 0.4 mM) caused a fall in SBP from 116 +/- 6 to 49 +/- 6 mmHg and in MAF from 373 +/- 30 to 181 +/- 53 ml/min (P < 0.01). Raising [K+]p (11.6 +/- 0.3 mM) with norepinephrine (NE) (1.3 micrograms.kg-1.min-1 iv), however, increased SBP from 108 +/- 7 to 150 +/- 6 mmHg (P < 0.01) and MAF from 347 +/- 42 to 434 +/- 35 ml/min (P < 0.01). In 19 isolated working hearts, perfusion with 8 mM K+ Tyrode and then 12 mM K+ Tyrode reduced MOP from 87 +/- 3 (control 4 mM K+) to 67 +/- 3 (8 mM K+) and 51 +/- 2 cmH2O (12 mM K+) (P < 0.01); 12 mM K+ Tyrode with 0.08 microM NE or epinephrine, however, increased MOP from 67 +/- 6 (in 8 mM K+) to 85 +/- 6 cmH2O (NE) and from 58 +/- 2 to 76 +/- 5 cmH2O (epinephrine) (P < 0.01). Catecholamines may therefore play a key role in protecting the heart from exercise-induced hyperkalemia.     

Permeability properties and intracellular ion concentrations of epithelial cells in rat duodenum.

Effects of the K+ concentration in the bathing fluid ([K+]l) on the intracellular K+, Na+ and Cl- concentrations ([K+]i [Na+]i and [Cl-]i) as well as on the electrical potential were studied in rat duodenum. Changes in the mucosal K+ concentration ([K+]m), bringing the sum of Na+ and K+ concentrations to 147.2 mM constant, had little effect on the transmural potential difference (PDt), but did induce marked changes in the mucosal membrane potential (Vm). As [K+]m increased, Vm was depolarized gradually and obeyed the Nernst equation for a potassium electrode in the range of [K+]m greater than approx. 60 mM. Experiments of ion analyses were carried out on strips of duodenum to determine the effect of changing the external K+ concentrations on [K+] i, [Na+]i and [Cl-]i. An increase in [K+]o resulted in increases in [K+]i and [Cl-]i and a decrease in [Na+]i, [K+]i approaching its maximum at [K+]o greater than 70 mM. Such changes in [K+]i and [Na+]i seem to correlate quantitatively with the changes in [K+]o and [Na+]o. The values of the ratio of permeability coefficients, Pna+/PK+ were estimated using the Vm values and intracellular ion concentrations measured in these experiments. The results suggested that there appeared a rather abrupt increase in the PNa+/PK+ ratio from 0 to approx. 0.1, as [K+]m decreased.     

Ion permeation and block of M-type and delayed rectifier potassium channels. Whole-cell recordings from bullfrog sympathetic neurons

Ion permeation and conduction were studied using whole-cell recordings of the M-current (I(M)) and delayed rectifier (IDR), two K+ currents that differ greatly in kinetics and modulation. Currents were recorded from isolated bullfrog sympathetic neurons with 88 mM [K+]i and various external cations. Selectivity for extracellular monovalent cations was assessed from permeability ratios calculated from reversal potentials and from chord conductances for inward current. PRb/PK was near 1.0 for both channels, and GRb/GK was 0.87 +/- 0.01 for IDR but only 0.35 +/- 0.01 for I(M) (15 mM [Rb+]o or [K+]o). The permeability sequences were generally similar for I(M) and IDR: K+ approximately Rb+ > NH4+ > Cs+, with no measurable permeability to Li+ or CH3NH3+. However, Na+ carried detectable inward current for IDR but not I(M). Nao+ also blocked inward K+ current for IDR (but not IM), at an apparent electrical distance (delta) approximately 0.4, with extrapolated dissociation constant (KD) approximately 1 M at 0 mV. Much of the instantaneous rectification of IDR in physiologic ionic conditions resulted from block by Nao+. Extracellular Cs+ carried detectable inward current for both channel types, and blocked I(M) with higher affinity (KD = 97 mM at 0 mV for I(M), KD) approximately 0.2 M at 0 mV for IDR), with delta approximately 0.9 for both. IDR showed several characteristics reflecting a multi-ion pore, including a small anomalous mole fraction effect for PRb/PK, concentration-dependent GRb/GK, and concentration- dependent apparent KD's and delta's for block by Nao+ and Cso+. I(M) showed no clear evidence of multi-ion pore behavior. For I(M), a two- barrier one-site model could describe permeation of K+ and Rb+ and block by Cso+, whereas for IDR even a three-barrier, two-site model was not fully adequate.     

The independence of membrane potential and potassium activation of the sodium pump in muscle.

The membrane potential (Em) of sartorius muscle fibers was made insensitive to [K+] by equilibration in a 95 mM K+, 120 mM Na+ Ringer solution. Under these conditions a potassium-activated, ouabain-sensitive sodium efflux was observed which had characteristics similar to those seen in muscles with Em sensitive to [K+]. In addition, in the presence of 10 mM K+, these muscles were able to produce a net sodium extrusion against an electrochemical gradient which was also inhibited by 10- minus 4 M oubain. This suggests that the membrane potential does not play a major role in the potassium activation of the sodium pump in muscles.     

The Gibbs-Donnan near-equilibrium system of heart

The gradients of the major inorganic ions across the plasma membrane of heart were examined to determine the factors controlling the extent and direction of the changes induced during injury, certain diseases, and electrolyte disturbances. The ionic environment was altered by changing only the concentration of inorganic phosphate, [sigma Pi]o, from 0 to 1.2 to 5 mM in the Krebs-Henseleit buffer perfusing working rat hearts. Raising [sigma Pi]o from 1.2 to 5 mM resulted in a decrease in total Mg2+ content and calculated free cytosolic [Mg2+] from 0.44 to 0.04 mM, conversion of 4 mmol of MgATP2- to ATP4- and a decrease in measured intracellular [Cl-]i from 41 to 16 mM. At all levels of [sigma Pi]o, both the [Na+]i and [K+]i were invariant at about 3 mM and 130 mM, respectively, as was the energy of hydrolysis of the terminal phosphate bond of sigma ATP, delta GATP Hydr, of -13.2 kcal/mol. The relationship maintained between the ions on both sides of the plasma membrane by the 3Na+/2K(+)transporting ATPase (EC 3.6.1.37) and an open K+ channel was: (formula; see text) The energy of the gradients of the other inorganic ions across the plasma membrane, delta G[ion]o/i, exhibited three distinct quanta of energy derived from the prime quantum of delta GATP Hydr of -13.2 kcal/mol. The second quantum was about one-third of delta GATP Hydr or +/- 4.4 kcal/mol and comprised the delta G[Na+]o/i, delta G[Mg2+]o/i, and delta G[HPO42-]o/i. These results indicated near-equilibrium was achieved by the reactants of the 3Na+/2K(+)-ATPase, the K+ channel, the Na(+)-Pi co-transporter, and a postulated net Mg2+/H2PO4- exchanger. The third quantum was one-third of delta G[Na+]o/i or about +/- 1.5 kcal/mol and comprised delta G[H+]o/i, delta G[HCO3-]o/i, and delta G[Cl-]o/i. The delta G[K+]o/i was 0, indicating near-equilibrium between the chemical energy of [K+]o/i and the E across the plasma membrane of -83 mV. It is concluded that the gradients of the major inorganic ions across the plasma membrane and the potential across that membrane constitute a Gibbs-Donnan equilibrium system catalyzed by transport enzymes sharing common substrates. The chemical and electrical energies of those gradients are equal in magnitude and opposite in sign to the chemical energy of ATP hydrolysis.     

Lymphocyte membrane potential and Ca2+-sensitive potassium channels described by oxonol dye fluorescence measurements

A method is described for quantitative measurement of lymphocyte transmembrane electrical potential difference (psi) by flow cytometric recording of the oxonol dye fluorescence of single cells. Both the simultaneous collection and analysis of multiple optical parameters and the use of a negatively charged oxonol probe allowed more accurate measurement of psi than may be obtained by bulk cell suspension techniques employing cationic voltage indicators. Mouse spleen and human blood lymphocyte psi was calculated to be -70 mV. T and B lymphocytes maintain a constant psi as extracellular K+ is varied from 2 to 10 mM and the deviation from K+ equilibrium potentials (EK) is shown to result from Na+ permeability. At [K+]o values greater than 10 mM, lymphocytes behave as K+ electrodes. Examination of lymphocyte subsets showed that hyperpolarization induced by the Ca2+ ionophore A23187 occurs only in T cells. This response was identified as activation of a Ca2+-sensitive K+ channel by pharmacologic manipulations. Hence, T cells depolarized by 4-aminopyridine (4-AP, 10 mM) were observed to return to resting psi by A23187-induced elevation of [Ca2+]i. Cells depolarized by quinine (100 microM) were unaffected by A23187. The Ca2+-activated channel does not contribute to resting psi in T cells since it may be selectively blocked by quinine (20 microM) or modulated by calmodulin antagonists (5 microM trifluperazine) without affecting resting psi.