Reaccumulation of [K+]o in the toad retina during maintained illumination

Using K+-selective microelectrodes, [K+]o was measured in the subretinal space of the isolated retina of the toad, Bufo marinus. During maintained illumination, [K+]o fell to a minimum and then recovered to a steady level that was approximately 0.1 mM below its dark level. Spatial buffering of [K+]o by Müller (glial) cells could contribute to this reaccumulation of K+. However, superfusion with substances that might be expected to block glial transport of K+ had no significant effect upon the reaccumulation of K+. These substances included blockers of gK (TEA+, Cs+, Rb+, 4-AP) and a gliotoxin (alpha AAA). Progressive slowing of the rods' Na+/K+ pump (perhaps caused by a light-evoked decrease in [Na+]i) also could contribute to this reaccumulation of K+ by reducing the uptake of K+ from the subretinal space. As evidence for a major contribution by this mechanism, treatments designed to prevent such slowing of the pump reversibly blocked reaccumulation. These treatments included superfusion with 2 microM ouabain, or lowering [K+]o, PO2, or temperature. It is likely that such treatments inhibit the pump, increase [Na+]i, and attenuate any light-evoked decrease in [Na+]i. The results are consistent with the following hypothesis. At light onset, the decrease in rod gNa will reduce the Na+ influx and the resulting rod hyperpolarization will reduce the K+ efflux. In combination with these reduced passive fluxes, the continuing active fluxes will lower both [K+]o and [Na+]i, which in turn will inhibit the pump. In support of this hypothesis, the solutions to a pair of coupled differential equations that model changes in both [K+]o and [Na+]i match quantitatively the time course of the observed changes in [K+]o during and after maintained illumination for all stimuli examined.     

Ba2+ unmasks K+ modulation of the Na+-K+ pump in the frog retinal pigment epithelium

This paper presents electrophysiological evidence that small changes in [K+]o modulate the activity of the Na+-K+ pump on the apical membrane of the frog retinal pigment epithelium (RPE). This membrane also has a large relative K+ conductance so that lowering [K+]o hyperpolarizes it and therefore increases the transepithelial potential (TEP). Ba2+, a K+ channel blocker, eliminated these normal K+-evoked responses; in their place, lowering [K+]o evoked an apical depolarization and TEP decrease that were blocked by apical ouabain or strophanthidin. These data indicate that Ba2+ blocked the major K+ conductance(s) of the RPE apical membrane and unmasked a slowing of the normally hyperpolarizing electrogenic Na+-K+ pump caused by lowering [K+]o. Evidence is also presented that [K+]o modulates the pump in the isolated RPE under physiological conditions (i.e., without Ba2+). In the intact retina, light decreases subretinal [K+]o and produces the vitreal-positive c-wave of the electroretinogram (ERG) that originates primarily in the RPE from a hyperpolarization of the apical membrane and TEP increase. When Ba2+ was present in the retinal perfusate, the apical membrane depolarized in response to light and the TEP decreased so that the ERG c-wave inverted. The retinal component of the c-wave, slow PIII, was abolished by Ba2+. The effects of Ba2+ were completely reversible. We conclude that Ba2+ unmasks a slowing of the RPE Na+-K+ pump by the light-evoked decrease in [K+]o. Such a response would reduce the amplitude of the normal ERG c-wave.     

Potassium and the photoreceptor-dependent pigment epithelial hyperpolarization

Light-evoked changes in pigment epithelial cell membrane potentials and retinal extracellular potassium ion concentration, [K+]0, were measured in an in vitro frog retina-pigment epithelium-choroid preparation. Light stimuli hyperpolarized the apical membrane of the pigment epithelium. Through an electrical shunt pathway connecting the apical and basal membranes, the basal membrane also hyperpolarized, but to a lesser degree than the apical membrane. This differential hyperpolariation of the two membranes increased the transepithelial potential (TEP). This increase in TEP was shown to be the major voltage source of the c-wave of the electroretinogram (ERG). Direct measurement of [K+]0 in the distal retina, made with K+-specific microelectrodes, showed a light-evoked decrease in [K+]0 having an identical time course to the apical hyperpolarization. There was a linear relationship between the light-evoked change in TEP and the logarithm of [K+]0. This exact relationship was also found when the apical membrane was perfused directly with solutions of varying [K+]0. The change in TEP associated with the ERC c-wave, therefore, was explained solely by the response of the pigment epithelium to the light-evoked decrease in [K+]0 in the distal retina.     

Sources and sinks of light-evoked delta [K+]o in the vertebrate retina

In the vertebrate retina, recordings of light-evoked changes in extracellular K+ concentration delta [K+]o are of particular interest because this tissue is complex and multilayered, yet can be activated routinely with its "natural" stimulus (i.e., light). This review identifies the components of the spatiotemporal profile of retinal light-evoked delta [K+]o and then presents evidence concerning the specific neural origins of these components as well as the mechanisms by which these delta [K+]o are dispersed from extracellular space. Finally, to gain improved resolution of K+ sources and sinks, the technique of ion source density is introduced and applied to both model and real spatiotemporal distributions of delta [K+]o.     

Plasma membrane hyperpolarization and [Ca2+]i increase induced by fibroblast growth factor in NIH-3T3 fibroblasts: resemblance to early signals generated by platelet-derived growth factor

The effects of different substances on [Ca2+]i and membrane potential (measured by fura-2 and bis-oxonol fluorescence techniques, respectively) were studied in wild-type and NIH-3T3 fibroblasts transfected with the cDNA encoding the human epidermal growth factor receptor. Application of partially purified PDGF or FGF induced, after a lag (0.5-1 min), a [Ca2+]i increase composed by an initial, slow peak, sustained primarily by intracellular Ca2+ release followed by a plateau, sustained by Ca2+ influx from the medium. The [Ca2+]i changes were paralleled by plasma membrane hyperpolarization mainly due to the activation of a K+ efflux, since raising the extracellular K+ concentration progressively reversed the effect of both growth factors. These responses were much slower than those induced by other agents (bradykinin, extracellular ATP, and EGF). The close resemblance between PDGF- and FGF-induced early signals (time-course and insensitivity to phorbol esters) suggests similar transmembrane signalling mechanisms at the cognate receptor.     

Changes in apical [K+] produce delayed basal membrane responses of the retinal pigment epithelium in the gecko

We describe here a new retinal pigment epithelium (RPE) response, a delayed hyperpolarization of the RPE basal membrane, which is initiated by the light-evoked decrease of [K+]o in the subretinal space. This occurs in addition to an apical hyperpolarization previously described in cat (Steinberg et al., 1970; Schmidt and Steinberg, 1971) and in bullfrog (Oakley et al., 1977; Oakley, 1977). Intracellular and extracellular potentials and measurements of subretinal [K+]o were recorded from an in vitro preparation of neural retina-RPE-choroid from the lizard Gekko gekko in response to light. Extracellularly, the potential across the RPE, the transepithelial potential (TEP), first increased and then decreased during illumination. Whereas the light- evoked decrease in [K+]o predicted the increase in TEP, the subsequent decrease in TEP was greater than predicted by the reaccumulation of [K+]o. Intracellular RPE recordings showed that a delayed hyperpolarization generated at the RPE basal membrane produced the extra TEP decrease. At light offset, the opposite sequence of membrane potential changes occurred. RPE responses to changes in [K+]o were studied directly in the isolated gecko RPE-choroid. Decreasing [K+]o in the apical bathing solution produced first a hyperpolarization of the apical membrane, followed by a delayed hyperpolarization of the basal membrane, a sequence of membrane potential changes identical to those evoked by light. Increasing [K+]o produced the opposite sequence of membrane potential changes. In both preparations, the delayed basal membrane potentials were accompanied by changes in basal membrane conductance. The mechanism by which a change in extracellular [K+] outside the apical membrane leads to a polarization of the basal membrane remains to be determined.     

Effects of hypoxia on potassium homeostasis and pigment epithelial cells in the cat retina

Intracellular recordings show that light-evoked hyperpolarizations of the apical and basal membranes of the cat retinal pigment epithelium (RPE) are altered by mild hypoxia. RPE cells, like glia, have a high K+ conductance, and measurements with K+-sensitive microelectrodes show that the hypoxic changes in the RPE cell are largely the result of changes in extracellular [K+] in the subretinal space [( K+]o) rather than direct effects on RPE cells. During hypoxia, light-evoked [K+]o responses and membrane responses have longer times to peak, slower and less complete recovery during illumination, and larger amplitudes. In addition to the effects on light-evoked responses, hypoxia causes a depolarization of first the apical and then the basal membranes of RPE cells under dark-adapted conditions. The basal depolarization is accompanied by a decrease in basal membrane resistance. These depolarizations appear to be caused by a rapid increase in [K+]o at the onset of hypoxia, which is maximal in dark adaptation, and smaller if the retina is subjected to maintained illumination. All of the effects are graded with the severity of hypoxia and can be observed at arterial oxygen tensions as high as 65 mmHg, although the threshold may be even higher. We argue that the origin of hypoxic [K+]o changes is probably an inhibition of the photoreceptors' Na+/K+ pump. This work then suggests that photoreceptors are more sensitive to hypoxia than previously believed, and that the high oxygen tension normally provided by the choroidal circulation is necessary for normal photoreceptor function.     

Decline of electrogenic Na+/K+ pump activity in rod photoreceptors during maintained illumination

Light-evoked changes in membrane voltage were recorded intracellularly from rod photoreceptors in the isolated retina preparation of the toad, Bufo marinus, during superfusion with a solution containing pharmacological agents that blocked voltage-dependent conductances. Under these conditions, the amplitude of the hyperpolarizing photoresponse became much greater than under control conditions. The results of several experiments support the conclusion that this increase in photoresponse amplitude was due primarily to a voltage that was produced when the electrogenic current from the rods' Na+/K+ pump flowed across an increased membrane resistance (Torre, V. 1982. Journal of Physiology. 333:315). At the onset of a period of continuous illumination, the rod membrane first hyperpolarized and then began to repolarize, and after 180 s of illumination, the membrane voltage had recovered by 60-72% of its initial hyperpolarization. There did not appear to be any significant decrease in rod membrane resistance associated with this repolarization. Both the enhanced hyperpolarization at light onset and the slow repolarization during maintained illumination were blocked by superfusion with 10.0 microM strophanthidin. These data support the hypothesis that the activity of the rods' Na+/K+ pump declines progressively during maintained illumination. It is likely that the decline in pump activity produces significant changes in [K+]o in the subretinal space during maintained illumination.     

Measurement of potassium turnover in rod photoreceptors in toad isolated retina using ion-selective microelectrodes

Ion-selective microelectrodes (ISMs) were used to measure the turnover of intracellular K+ (Ki+) in rods in the isolated retina of the toad, Bufo marinus. The light-evoked hyperpolarization of rods decreases their passive K+ efflux, which in combination with active K+ uptake, decreases extracellular K+ concentration, Ko+.Rb+ substitutes for K+ in these processes. The turnover of Ki+ was measured as Rb+ and K+ were exchanged, using ISMs that were approximately five times more sensitive to Rb+ than to K+. When Ko+ was replaced by Rbo+, the light-evoked decrease in K+ efflux produced only a small change in ISM voltage, delta VISM, owing to the background of Rbo+. As Rbi+ replaced Ki+, the efflux shifted from K+ to Rb+ and delta VISM grew in amplitude. After loading the rods with Rbi+, Rbo+ was replaced by Ko+. The light-evoked decrease in Rb+ efflux lead transiently to a large delta VISM, since the change in Rbo+ was superimposed upon a background of Ko+. As Ki+ replaced Rbi+, the amplitude of delta VISM declined. When measured using this technique, the turnover of Ki+ was 95% complete in approximately 15 min. In low Ca2+ solutions, transmembrane fluxes of K+ (Rb+) increased and turnover of Ki+ occurred more rapidly. During background illumination, transmembrane fluxes of K+ (Rb+) decreased and turnover of Ki+ was slowed. These experiments have provided independent corroboration of earlier observations concerning rod K+ fluxes. This ISM-based technique also may be useful in measuring K+ turnover in other cell types.     

The role of K+ in the regulation of the increase in intracellular Ca2+ mediated by the T lymphocyte antigen receptor

The regulation of the increase in intracellular calcium ([Ca2+]i) occurring in cytolytic T lymphocytes (CTLs) upon their interaction with antigen was examined. This [Ca2+]i increase and lytic function were insensitive to verapamil, a Ca channel blocker. An antigen-independent increase in [Ca2+]i was not induced by depolarization of CTLs with excess extracellular K+, suggesting that Ca2+ influx is not mediated by the ubiquitous voltage-gated Ca channel. The antigen-induced [Ca2+]i increase was inhibited by prior membrane hyperpolarization with valinomycin. Hyperpolarization occurred under normal circumstances in CTLs exposed to antigen-receptor-specific antibodies. This potential change was Ca2+-dependent and inhibited by K channel blockade. Conversely, K channel blockade augmented the antigen-specific [Ca2+]i increase while markedly decreasing the K+ efflux associated with CTL lytic function. Therefore, either membrane potential or intracellular K+ regulates the antigen-specific [Ca2+]i increase in CTLs.     

Characterization of the cyclic AMP-independent actions of somatostatin in GH cells. I. An increase in potassium conductance is responsible for both the hyperpolarization and the decrease in intracellular free calcium produced by somatostatin

The neuropeptide somatostatin causes membrane hyperpolarization and reduces the intracellular free calcium ion concentration ([Ca2+]i) in GH pituitary cells. In this study, we have used the fluorescent dyes bisoxonol (bis,-(1,3-diethylthiobarbiturate)-trimethineoxonol) and quin2 to elucidate the mechanisms by which these ionic effects are triggered. Addition of 100 nM somatostatin to GH4C1 cells caused a 3.4 mV hyperpolarization and a 26% decrease in [Ca2+]i within 30 s. These effects were not accompanied by changes in intracellular cAMP concentrations and occurred in cells containing either basal or maximally elevated cAMP levels. To determine which of the major permeant ions were involved in these actions of somatostatin, we examined its ability to elicit changes in the membrane potential and the [Ca2+]i when the transmembrane concentration gradients for Na+, Cl-, Ca2+, and K+ were individually altered. Substitution of impermeant organic ions for Na+ or Cl- did not block either the hyperpolarization or the decrease in [Ca2+]i induced by somatostatin. Decreasing extracellular Ca2+ from 1 mM to 250 nM abolished the reduction in [Ca2+]i but did not prevent the hyperpolarization response. These results show that hyperpolarization was not primarily due to changes in the conductances of Na+, Cl-, or Ca2+. Although the somatostatin-induced decrease in [Ca2+]i did require Ca2+ influx, it was independent of changes in Na+ or Cl- conductance. In contrast, elevating the extracellular [K+] from 4.6 to 50 mM completely blocked both the somatostatin-induced hyperpolarization and the reduction in [Ca2+]i. Furthermore, hyperpolarization of the cells with gramicidin mimicked the effect of somatostatin to decrease the [Ca2+]i and prevented any additional effect by the hormone. These results indicate that somatostatin increases a K+ conductance, which hyperpolarizes GH4C1 cells, and thereby secondarily decreases Ca2+ influx. Since the somatostatin-induced decrease in [Ca2+]i is independent of changes in intracellular cAMP levels, it may be responsible for somatostatin inhibition of hormone secretion by its cAMP-independent mechanism.     

Kinetics and stoichiometry of coupled Na efflux and Ca influx (Na/Ca exchange) in barnacle muscle cells

Coupled Na+ exit/Ca2+ entry (Na/Ca exchange operating in the Ca2+ influx mode) was studied in giant barnacle muscle cells by measuring 22Na+ efflux and 45Ca2+ influx in internally perfused, ATP-fueled cells in which the Na+ pump was poisoned by 0.1 mM ouabain. Internal free Ca2+, [Ca2+]i, was controlled with a Ca-EGTA buffering system containing 8 mM EGTA and varying amounts of Ca2+. Ca2+ sequestration in internal stores was inhibited with caffeine and a mitochondrial uncoupler (FCCP). To maximize conditions for Ca2+ influx mode Na/Ca exchange, and to eliminate tracer Na/Na exchange, all of the external Na+ in the standard Na+ sea water (NaSW) was replaced by Tris or Li+ (Tris-SW or LiSW, respectively). In both Na-free solutions an external Ca2+ (Cao)-dependent Na+ efflux was observed when [Ca2+]i was increased above 10(-8) M; this efflux was half-maximally activated by [Ca2+]i = 0.3 microM (LiSW) to 0.7 microM (Tris-SW). The Cao-dependent Na+ efflux was half-maximally activated by [Ca2+]o = 2.0 mM in LiSW and 7.2 mM in Tris-SW; at saturating [Ca2+]o, [Ca2+]i, and [Na+]i the maximal (calculated) Cao-dependent Na+ efflux was approximately 75 pmol#cm2.s. This efflux was inhibited by external Na+ and La3+ with IC50's of approximately 125 and 0.4 mM, respectively. A Nai-dependent Ca2+ influx was also observed in Tris-SW. This Ca2+ influx also required [Ca2+]i greater than 10(-8) M. Internal Ca2+ activated a Nai-independent Ca2+ influx from LiSW (tracer Ca/Ca exchange), but in Tris-SW virtually all of the Cai-activated Ca2+ influx was Nai-dependent (Na/Ca exchange). Half-maximal activation was observed with [Na+]i = 30 mM. The fact that internal Ca2+ activates both a Cao-dependent Na+ efflux and a Nai-dependent Ca2+ influx in Tris-SW implies that these two fluxes are coupled; the activating (intracellular) Ca2+ does not appear to be transported by the exchanger. The maximal (calculated) Nai-dependent Ca2+ influx was -25 pmol/cm2.s. At various [Na+]i between 6 and 106 mM, the ratio of the Cao-dependent Na+ efflux to the Nai-dependent Ca2+ influx was 2.8-3.2:1 (mean = 3.1:1); this directly demonstrates that the stoichiometry (coupling ratio) of the Na/Ca exchange is 3:1. These observations on the coupling ratio and kinetics of the Na/Ca exchanger imply that in resting cells the exchanger turns over at a low rate because of the low [Ca2+]i; much of the Ca2+ extrusion at rest (approximately 1 pmol/cm2.s) is thus mediated by an ATP-driven Ca2+ pump.(ABSTRACT TRUNCATED AT 400 WORDS)     

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.     

The nss mutation or lanthanum inhibits light-induced Ca2+ influx into fly photoreceptors.

Ion-selective calcium microelectrodes were inserted into the compound eyes of the wild-type sheep blowfly Lucilia or into the retina of the no steady state (nss) mutant of Lucilia. These electrodes monitored light-induced changes in the extracellular concentration of calcium (delta[Ca2+]o) together with the extracellularly recorded receptor potential. Prolonged dim lights induced a steady reduction in [Ca2+]o during light in the retina of normal Lucilia, while relatively little change in [Ca2+]o was observed in the retina of the nss mutant. Prolonged intense light induced a multiphasic change in [Ca2+]o: the [Ca2+]o signal became transient, reaching a minimum within 6 s after light onset, and then rose to a nearly steady-state phase below the dark concentration. When lights were turned off, a rapid increase in [Ca2+]o was observed, reaching a peak above the dark level and then declining again to the dark level within 1 min. In analogy to similar studies conduced in the honeybee drone, we suggest that the reduction in [Ca2+]o reflects light-induced Ca2+ influx into the photoreceptors, while the subsequent increase in [Ca2+]o reflects the activation of the Na-Ca exchange which extrudes Ca2+ from the cells. In the nss mutant in response to intense prolonged light, the receptor potential declines to baseline during light while the Ca2+ signal is almost abolished, revealing only a short transient reduction in [Ca2+]o. Application of lanthanum (La3+), but not nickel (Ni2+), into the retinal extracellular space of normal Lucilia mimicked the effect of the nss mutation on the receptor potential, while complete elimination of the Ca2+ signal in a reversible manner was observed. The results suggest that La3+ and the nss mutation inhibit light-induced Ca2+ influex into the photoreceptor in a manner similar to the action of the trp mutation in Drosophila, which has been shown to block specifically a light-activated Ca2+ channel necessary to maintain light excitation.     

Genetic dissection of light-induced Ca2+ influx into Drosophila photoreceptors

Invertebrate photoreceptors use the inositol-lipid signaling cascade for phototransduction. A useful approach to dissect this pathway and its regulation has been provided by the isolation of Drosophila visual mutants. We measured extracellular changes of Ca2+ [delta Ca2+]o in Drosophila retina using Ca(2+)-selective microelectrodes in both the transient receptor potential (trp) mutant, in which the calcium permeability of the light-sensitive channels is greatly diminished and in the inactivation-but-no-afterpotential C (inaC) mutant which lacks photoreceptor-specific protein kinase C (PKC). Illumination induced a decrease in extracellular [Ca2+] with kinetics and magnitude that changed with light intensity. Compared to wild-type, the light-induced decrease in [Ca2+]o (the Ca2+ signal) was diminished in trp but significantly enhanced in inaC. The enhanced Ca2+ signal was diminished in the double mutant inaC;trp indicating that the effect of the trp mutation overrides the enhancement observed in the absence of eye-PKC. We suggest that the decrease in [Ca2+]o reflects light-induced Ca2+ influx into the photoreceptors and that the trp mutation blocks a large fraction of this Ca2+ influx, while the absence of eye specific PKC leads to enhancement of light-induced Ca2+ influx. This suggestion was supported by Ca2+ measurements in isolated ommatidia loaded with the fluorescent Ca2+ indicator, Ca Green-5N, which indicated an approximately threefold larger light-induced increase in cellular Ca2+ in inaC relative to WT. Our observations are consistent with the hypothesis that TRP is a light activated Ca2+ channel and that the increased Ca2+ influx observed in the absence of PKC is mediated mainly via the TRP channel.     

Rapid, futile K+ cycling and pool-size dynamics define low-affinity potassium transport in barley

Using the short-lived radiotracer 42K+, we present a comprehensive subcellular flux analysis of low-affinity K+ transport in plants. We overturn the paradigm of cytosolic K+ pool-size homeostasis and demonstrate that low-affinity K+ transport is characterized by futile cycling of K+ at the plasma membrane. Using two methods of compartmental analysis in intact seedlings of barley (Hordeum vulgare L. cv Klondike), we present data for steady-state unidirectional influx, efflux, net flux, cytosolic pool size, and exchange kinetics, and show that, with increasing external [K+] ([K+]ext), both influx and efflux increase dramatically, and that the ratio of efflux to influx exceeds 70% at [K+]ext > or = 20 mm. Increasing [K+]ext, furthermore, leads to a shortening of the half-time for cytosolic K+ exchange, to values 2 to 3 times lower than are characteristic of high-affinity transport. Cytosolic K+ concentrations are shown to vary between 40 and 200 mm, depending on [K+]ext, on nitrogen treatment (NO3- or NH4+), and on the dominant mode of transport (high- or low-affinity transport), illustrating the dynamic nature of the cytosolic K+ pool, rather than its homeostatic maintenance. Based on measurements of trans-plasma membrane electrical potential, estimates of cytosolic K+ pool size, and the magnitude of unidirectional K+ fluxes, we describe efflux as the most energetically demanding of the cellular K+ fluxes that constitute low-affinity transport.     

Physiological implications of K accumulation in heart muscle

K+-selective microelectrodes in conjugation with the voltage clamp technique were used to examine the voltage and time dependence of K+ efflux and accumulation in cardiac muscle. K+ efflux per action potential is about 10 to 30 pmoles/cm2 per sec. Accumulation of K+ in the paracellular space plays an important role in regulation of action potential duration, so that the [K+]o prior to generation of an action potential determines the duration of following action potential. This regulation is brought about by the shift of inward rectifying K+ current along the voltage axis, so at higher [K+]o there is more outward current at plateau potentials. Monitoring [K+]o after a period of rapid beating provides quantitative data regarding Na-pump activity. The data suggest the Na-pump is electrogenic, making it difficult to assess the extent of K+ accumulation from the measurements of resting potential alone. These studies indicate that changes in [K+]o not only reflect outward membrane currents and Na-pump activity, but also play an important physiological regulatory role in determining the duration of the action potential.     

Electrophysiological effects of basolateral [Na+] in Necturus gallbladder epithelium

In Necturus gallbladder epithelium, lowering serosal [Na+] ([Na+]s) reversibly hyperpolarized the basolateral cell membrane voltage (Vcs) and reduced the fractional resistance of the apical membrane (fRa). Previous results have suggested that there is no sizable basolateral Na+ conductance and that there are apical Ca(2+)-activated K+ channels. Here, we studied the mechanisms of the electrophysiological effects of lowering [Na+]s, in particular the possibility that an elevation in intracellular free [Ca2+] hyperpolarizes Vcs by increasing gK+. When [Na+]s was reduced from 100.5 to 10.5 mM (tetramethylammonium substitution), Vcs hyperpolarized from -68 +/- 2 to a peak value of -82 +/- 2 mV (P less than 0.001), and fRa decreased from 0.84 +/- 0.02 to 0.62 +/- 0.02 (P less than 0.001). Addition of 5 mM tetraethylammonium (TEA+) to the mucosal solution reduced both the hyperpolarization of Vcs and the change in fRa, whereas serosal addition of TEA+ had no effect. Ouabain (10(-4) M, serosal side) produced a small depolarization of Vcs and reduced the hyperpolarization upon lowering [Na+]s, without affecting the decrease in fRa. The effects of mucosal TEA+ and serosal ouabain were additive. Neither amiloride (10(-5) or 10(-3) M) nor tetrodotoxin (10(-6) M) had any effects on Vcs or fRa or on their responses to lowering [Na+]s, suggesting that basolateral Na+ channels do not contribute to the control membrane voltage or to the hyperpolarization upon lowering [Na+]s. The basolateral membrane depolarization upon elevating [K+]s was increased transiently during the hyperpolarization of Vcs upon lowering [Na+]s. Since cable analysis experiments show that basolateral membrane resistance increased, a decrease in basolateral Cl- conductance (gCl-) is the main cause of the increased K+ selectivity. Lowering [Na+]s increases intracellular free [Ca2+], which may be responsible for the increase in the apical membrane TEA(+)-sensitive gK+. We conclude that the decrease in fRa by lowering [Na+]s is mainly caused by an increase in intracellular free [Ca2+], which activates TEA(+)-sensitive maxi K+ channels at the apical membrane and decreases apical membrane resistance. The hyperpolarization of Vcs is due to increase in: (a) apical membrane gK+, (b) the contribution of the Na+ pump to Vcs, (c) basolateral membrane K+ selectivity (decreased gCl-), and (d) intraepithelial current flow brought about by a paracellular diffusion potential.     

Non-pumped sodium fluxes in human red blood cells. Evidence for facilitated diffusion.

Unidirectional and net Na+ fluxes modified by changes in internal Na+ concentration ([Na+]i) were studied in human red blood cells incubated in K+-free solutions containing 10-minus 4 m ouabain. An increase in [Na+]i brought about (a) a reduction in net Na+ gain, (b) no change in Na+ influx, (c) a reduction in the rate constant for Na+ effux and (d) an increase in Na+ efflux. Similar reductions in net Na+ gain were observed when the changes in [Na+]i were carried out at constant [K+]i. In addition, the rate constant for 42K+ efflux was not affected by changes in [Na+]i. The electrical membrane potential (as determined from the chloride distribution ratio) was also constnat. Furosemide (10-minus 3 M) increased the net Na+ gain in concentration reduced Na+ efflux and increased Na+ influx: the magnitude of these effects was dependent onthe intracellular Na+. The reduction in the net Na+ gain as [Na+]i increased was unaffected by depletion of cellular ATP to values below 10 mumol/1 cells, and this effect was independent of the depletion method used     

Changes in internal ionized Ca2+ and H+ in voltage clamped squid axons

Squid giant axons were injected with aequorin and tetraethylammonium and were impaled with hydrogen ion sensitive, current and voltage electrodes. A newly designed horizontal microinjector was used to introduce the aequorin. It also served, simultaneously, as the current and voltage electrode for voltage clamping and as the reference for ion-sensitive microelectrode measurements. The axons were usually bathed in a solution containing 150 mM each of Na+, K+, and some inert cation, at either physiological or zero bath Ca2+ concentration [( Ca2+]o), and had ionic currents pharmacologically blocked. Voltage clamp pulses were repeatedly delivered to the extent necessary to induce a change in the aequorin light emission, a measure of axoplasmic ionized Ca2+ level, [( Ca2+]i). Alternatively, membrane potential was steadily held at values that represented deviations from the resting membrane potential observed at 150 mM [K+]o (i.e. approximately -15 mV). In the absence of [Ca2+]o a significant steady depolarization brought about by current flow increased [Ca2+]i (and acidified the axoplasm). Changes in internal hydrogen activity, [H+]i, induced by current flow from the internal Pt wire limited the extent to which valid measurements of [Ca2+]i could be made. However, there are effects on [Ca2+]i that can be ascribed to membrane potential. Thus, in the absence of [Ca2+]o, hyperpolarization can reduce [Ca2+]i, implying that a Ca2+ efflux mechanism is enhanced. It is also observed that [Ca2+]i is increased by depolarization. These results are consistent with the operation of an electrogenic mechanism that exchanges Na+ for Ca2+ in squid giant axon.