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The influence of cellular amino acids and the Na+ : K+ pump on the membrane potential of the Ehrlich ascites tumor cell.

The membrane potential of the Ehrlich ascites tumor cell was shown to be influenced by its amino acid content and the activity of the Na+ :K+ pump. The membrane potential (monitored by the fluorescent dye, 3,3'-dipropylthiodicarbocyanine iodide) varied with the size of the endogenous amino acid pool and with the concentration of accumulated 2-aminoisobutyrate. When cellular amino acid content was high, the cells were hyperpolarized; as the pool declined in size, the cells were depolarized. The hyperpolarization seen with cellular amino acid required cellular Na+ but not cellular ATP. Na+ efflux was more rapid from cells containing 2-aminoisobutyrate than from cells low in internal amino acids. These observations indicate that the hyperpolarization recorded in cells with high cellular amino acid content resulted from the electrogenic co-efflux of Na+ and amino acids. Cellular ATP levels were found to decline rapidly in the presence of the dye and hence the influence of the pump was seen only if glucose was added to the cells. When the cells contained normal Na+ (approx. 30mM), the Na+ :K+ pump was shown to have little effect on the membrane potential (the addition of ouabain had little effect on the potential). When cellular Na+ was raised to 60mM, the activity of the pump changed the membrane potential from the range -25 to -30 mV to -44 to -63 mV. This hyperpolarization required external K+ and was inhibited by ouabain.

Amino Acids

Potential difference and the distribution of ions across the human red blood cell membrane; a study of the mechanism by which the fluorescent cation, diS-C3-(5) reports membrane potential.

1. The mechanism by which the fluorescent, cationic dye diS-C3-(5) responds to the membrane potential of red blood cells has been investigated. 2. The dye in aqueous solution absorbs most strongly at 650 nm. Addition of white, haemoglobin-free membranes red shifts the absorption maximum ca. 20 nm, while addition of membrane-free cell lysate results in the appearance of a new dye absorption peak at 590 nm. Thus the dye binds both to cell membranes and to cell contents. The component of the cytoplasm which binds the dye is non-dialysable, presumably haemoglobin. 3. Dye added to a suspension of intact cells shows a strong absorption at 590 nm indicating that the dye has bound to the cell contents and that the membrane is permeable to the dye. 4. The amount of dye which partitions into (and on to) the cells can be determined, as reported by Sims, Waggoner, Wang & Hoffman (1974), from the fluorescence of the dye remaining in the supernatant after the cells are centrifuged to the bottom of the suspension. In most conditions the proportion of the cell associated dye which is either free inside the cell or bound to the outside face of the membrane is negligible compared to the proportion bound to the cell contents. 5. On the assumption that the dye is not actively transported, the ratio of the equilibrium dye activities inside and outside the cell, ai/ao, is determined by the membrane potential according to the Nernst relation. Driving the membrane potenial negative then increases the cell associated dye by increasing the activity ratio and hence ai and the amount of dye bound to cell contents. 6. At the known Donnan equilibrium potential the internal dye activity can be calculated from the external activity. An empirical relation between cell associated dye and internal activity has been determined by measuring the dye partition between cells and medium at different external activities. 7. Using this empirial relation, and providing that any changes in cell composition do not affect the dye binding, the internal activity at any potential can be calculated from the measured amount of cell associated dye. The external activity can be estimated fluorimetrically. The membrane potential is then calculated from the activity ratio. 8. The membrane potenial of cells has been altered by adding valinomycin in the presence of different K gradients. Under the conditions used, the 'constant field' permeability for K-Val is 15-20 times that of Cl. 9. Dye binding to haemoglobin is influenced by pH and thus dye partitioning into cells changes with intracellular pH. Increasing intracellular pH increases the amount of dye partitioned, while decreasing pH decreases this amount. 10. When large potentials are produced with valinomycin there is no change in intracellular pH. This result indicates that in red blood cells intracellular pH is determined by the external pH and the Cl concentration ratio and not by the membrane potentials. 11. DiS-C3-(5) can be used to estimate potentials across resealed ghost membranes...

Chlorides

Pancreatic acinar cells: effects of micro-ionophoretic polypeptide application on membrane potential and resistance.

1. Acinar cell membrane potential and resistance were measured from superfused segments of mouse pancreas, in vitro, using intracellular glass micro-electrodes. One or two extracellular micropipettes containing caerulein, bombesin nonapeptide (Bn) or acetylcholine (ACh) were placed near to the surface of the impaled acinus. The secretagogues were ejected rapidly from the micropipettes by ionophoresis.2. Each secretagogue evoked a similar electrical response from the impaled acinar cell: membrane depolarization and a simultaneous reduction in input resistance. The duration of cell activation from caerulein ionophoresis was longer than that observed for ACh and Bn. The cell response to the peptide hormone applications could be repeated in the presence of atropine.3. The minimum interval before the onset of cell depolarization after caerulein ionophoresis was determined. Values ranged between 500 and 1000 msec. The minimum latencies after Bn ionophoresis were 500-1400 msec.4. With two electrodes inserted into electrically coupled acinar cells, direct measurements of the caerulein and Bn null potentials were made. At high negative membrane potentials an enhanced depolarization was evoked by caerulein ionophoresis. At low negative membrane potentials the caerulein stimulation produced a diminished depolarization, and at membrane potentials less than - 10 mV acinar cell hyperpolarizations were observed. A similar series of responses was obtained in experiments where Bn ionophoresis was used. The caerulein and the Bn null potentials were always contained within - 10 to - 15 mV.5. The results describe the almost identical electrical response of acinar cells to stimulation by ACh, caerulein and bombesin. All three secretagogues have similar null potentials and latencies of activation on acinar cells. The bombesin latency responses appear as short as those measured for caerulein and provide electro-physiological evidence that Bn acts directly on acinar cells. The findings support the hypothesis that ACh, caerulein and Bn, though acting on different receptors, evoke the observed changes in electrical properties of acinar cell membranes, through a common pathway.

Acetylcholine

The membrane potential of rat diaphragm muscle fibres and the effect of denervation.

1. Resting membrane potentials of rat diaphragm muscles were measured in vitro after previous denervation for 0-10 days. In some experiments denervated muscles were incubated in vitro for 3 hr while in others they were cultured for 15-24 hr to allow adequate exposure to drugs before recording. 2. It was found that resting membrane potentials, within 2-5 mm of the site of nerve section were significantly lower, within 3 hr, than resting membrane potentials measured more than 9 mm away from site of nerve section. This difference could be reduced or abolished by bathing preparations in solutions containing adrenaline (10 muM), noradrenaline (10 muM) or isoprenaline (10 muM) or dibutyryl cyclic AMP (10 muM-0-25 mM in the presence of 2 mM theophylline). Cyclic AMP (0-5 mM) was ineffective. 3. Application of solutions containing dibutyryl cyclic AMP for 3 hr also raised the resting membrane potential of muscles denervated 4-5 days previously. Culture studies showed that this effect was sustained when the time of incubation was 24 hr. 4. Incubating freshly denervated preparations with cycloheximide (22 mug/ml.) or actinomycin D (1 mug/ml.) did not prevent the development of the early (3 hr) fall in resting membrane potential despite a concomitant inhibition of RNA or protein synthesis. Culturing freshly denervated muscles in solutions containing cycloheximide (10 or 25 mug/ml.) which blocked 93% of protein synthesis, did not prevent the expected drop in resting membrane potential after 15 or 24 hr. 5. It was found that exposure to ouabain (1 or 5 mM) produced a rapid (15 min) fall in resting membrane potential in innervated and denervated preparations treated with dibutyryl cyclic AMP but not denervated preparations. After 5 days denervation cyclic AMP levels in muscle were increased by about 40%. 6. It is suggested that upon denervation an electrogenic action of a NA+-pump is blocked and that dibutyryl cyclic AMP and catecholamines are capable of stimulating this pump.

Animals

Effect of inhibitors of aerobic and anaerobic metabolism on the membrane potential oscillation induced by veratrine.

1. Veratrine-induced membrane potential oscillation is still apparent after the muscle has been treated with 1 mM KCN, or 1 mM NaN3, or 0.2 mM DNP, to inhibit oxidative metabolism. 2. The frequency of the membrane potential oscillation decreases reversibly in response to 1 mM phlorrhizin either in Na- or Li-Ringer solution. 3. Veratrine causes no membrane potential oscillation but only depolarization in muscles pretreated with 0.5 mM iodoacetic acid, eventually a few abortive waves can be observed. Iodoacetic acid also abolishes oscillation which has already developed. 4. On the basis of the present data it is suggested that rhythmic changes of metabolism may be related to the oscillation of membrane potential.

Aerobiosis

Evidence for membrane potential changes in isolated synaptic membrane ghosts monitored with a merocyanine dye.

Changes in the fluorescence intensity of merocyanine-540 were measured in suspensions of synaptic plasma membrane ghosts isolated from rat brain cortex. With preincubation of the membrane ghosts in isotonic KCl or NaCl solution, K- and Na-enriched ghosts samples were prepared. In suspensions of both sort of synaptic membrane ghosts, merocyanine-540 showed a fluorescnece emission peak at a wavelength of 590 nm. Under a fixed total concentration of NaCl and KCl, high external K+ induced an increase in the fluorescence intensity, such an increase being proportional to logarithm of K+ concentration. Replacing K+ by Rb+, NH4+ or Cs+, a similar effect was observed. Rb+ was about as effective as K+ ; NH4 is about 2/3 and Cs+ 1/4 as effective. But the changes in fluorescence with increasing K+ concentration were larger in K-ghosts than in Na-ghosts. K+-induced fluorescence changes were very small when gramicidin D was added to the suspension. K+-induced fluorescence changes were not observed in ultrasonicated ghost suspensions. Such findings seem to indicates that the K+-ions induced fluorescence increase reflect the depolarization in the isolated synaptic plasma membrane ghosts. Furthermore, the permeability ratio PNa/PK (PNa, PK: the permeability constant for Na+ and K+) was estimated to be smaller than 0.03.

Animals

The dependence of membrane potential on extracellular chloride concentration in mammalian skeletal muscle fibres.

1. The steady-state intracellular membrane potential of fibres in thin bundles dissected from mouse extensor digitorum longus or soleus muscles or rat sternomastoid muscles was measured with 3 M-KCl glass micro-electrodes. The steady-state membrane potential was found to depend on the extracellular concentrations of Na, K and Cl ions. 2. The resting membrane potential (3.5 mM-[K]o, 160 mM-[Cl]o) was -74 +/- 1 mV (mean +/- S.E.) and a reduction in [Cl]o to 3.5 mM caused a reversible steady-state hyperpolarization to -94 +/- 1 mV (mean +/- S.E.). 3. The steady-state membrane potentials recorded in fibres exposed to different [K]o and zero [Cl]o were consistent with potentials predicted by the Goldman, Hodgkin & Katz (GHK) equation for Na and K. The results of similar experiments done with Cl as the major external anion could not be fitted by the same equation. 4. The GHK equation for Na, K and Cl did fit data obtained from fibres in solutions containing different [K]o with Cl as the major external anion if the intracellular Cl concentration was allowed to be out of equilibrium with the steady-state membrane potential. 5. It is suggested that an active influx of Cl ions controls the intracellular Cl concentrations in these fibres and hence maintains the Cl equilibrium potential at a depolarized value with respect to the resting membrane potential. 6. The steady-state membrane potential of rat diaphragm fibres was independent of [Cl]o and it seems likely that the intracellular Cl concentration of these fibres is not controlled by active Cl transport.

Animals

Change in membrane potential during bacterial chemotaxis.

To find out if there are changes in membrane potential during bacterial chemotaxis, we measured the membrane potential of Escherichia coli indirectly by use of the permeating, lipid-soluble cation triphenylmethylphosphonium. Addition of attractants or repellents to the bacteria brought about a hyperpolarizing peak (as well as additional, later changes in membrane potential). This peak was shown to be a part of the chemotactic mechanism based on the following evidence: (i) All attractants and repellents tested gave this peak while chemotactically inert chemicals did not. (ii) Mutants lacking galactose taxis failed to give the peak with galactose but did with another attractant and with repellents. (iii) Methionine, required for chemotaxis, is also required for production of this peak. (iv) A mutant in a control gene )flaI), unable to synthesize flagella and cytoplasmic membrane proteins related to motility and chemotaxis, failed to give the peak. (v) Paralyzed (mot) mutants gave little or none of the peak. Generally nonchemotactic (che) mutants, on the other hand, did give this peak. Very likely there are ion fluxes that bring about this change in membrane potential. We discuss the possible role of the mot gene product as an ion gate controlled by a methylation-demethylation process in response to attractants and repellents acting through their chemoreceptors.

Chemotaxis

Pancreatic acinar cells: effect of acetylcholine, pancreozymin, gastrin and secretin on membrane potential and resistance in vivo and in vitro.

1. Intracellular recordings of membrane potential and input resistance have been made in vivo and in vitro from the exocrine acinar cells of rat pancreas using indwelling glass micro-electrodes. 2. The resting cell membrane potential and input resistance in the in vivo experiments were not markedly different from the values obtained in the in vitro experiments. The effect of both acetylcholine (ACh) and pancreozymin (CCK-Pz) on the pancreas in vivo as well as in vitro was to reduce both the acinar cell membrane potential and the input resistance narkedly. The amplitude of the evoked depolarization and the change in input resistance evoked by supramaximal stimuli were of the same magnitude in both types of preparations. 3. Gastrin had an effect on the acinar cell potential and resistance which was indistinguishable from that of CCK-Pz or ACh. The effect of gastrin or CCK-Pz was, in contrast to that of ACh, not influenced by the presence of atropine. The reversal potential for the gastrin evoked potential change was about -20 mV. 4. Secretin in doses producing maximal volume secretion in vivo had no effect on acinar cell membrane potential and input resistance. 5. Dibutyryl cyclic AMP (5mM) and cyclic GMP (1mM) had no effect on cell membrane potential or resistance. 6. It is concluded that the in vitro superfused pancreas segment preparation is a useful model system in electrophysiological studies since it functions essentially as the in vivo preparation. In contrast to both gastrin and CCK-Pz, secretin has no effect on the bioelectrical properties of the acinar cells, indicating that there are no physiologically important secretin receptors in rat acinar cells.

Acetylcholine

Reflex effects and postsynaptic membrane potential changes during epileptiform activity induced by penicillin in decapitate spinal cords.

The administration of a convulsant dose of penicillin enhanced the transmission of monosynaptic reflexes in spinal cords in which reflex transmission was feeble before the drug treatment, but it had little effect in cords where monosynaptic reflexes were powerful to begin with. Post-tetanic potentiation was not altered by penicillin. Polysynaptic reflexes were invariably enhanced by convulsant amounts of penicillin. Postsynaptic ("direct") inhibition was not affected in the seizure-free intervals in spinal cords treated with penicillin, but it seemed to be suppressed during tonic seizures. The disability of reflex inhibition during ictal discharges may be due to presynaptic depolarization of inhibitory terminals. Recurrent inhibition was partially suppressed in spinal cords treated with penicillin. Neurons in the dorsal and intermediate gray matter were sometimes excited, sometimes inhibited, and sometimes unaffected by seizure activity of their segment. Motoneurons in the ventral horns invariably participated in the interictal and ictal activity. The timing of clonic seizure sequences coincided with bursts of Renshaw cell discharges. Action potential of abnormal amplitude and configuration were frequently observed in convulsing motoneurons. Paroxysmal depolarizing shifts (PDSs) of motoneurons were similar to those observed by other investigators in neurons in experimental epileptic foci of the cerebral cortex, except that spinal PDSs were not followed by hyperpolarizing waves.

Animals

Contribution of an electrogenic sodium pump to the membrane potential in the intestinal epithelial cell.

The transmural potential difference of isolated rat duodenum and the membrane potential of its epithelial cell were examined during changes of the ionic medium at both warm (31--35 degrees C) and cold temperatures (2--5 degrees C). In the range of low external K+ concentrations, cooling produced an immediate and reversible depolarization of the membrane potential (around -10 mV) greater than that estimated from a simple thermodynamic temperature effect (RT/F). Such a temperature sensitive component of the membrane potential at 31 degrees C was completely abolished by anoxia and serosal ouabain. Readmission of K+ to the bathing fluid of duodenum previously deprived of K+ and loaded by Na+ caused a remarkable transient hyperpolarization of the epithelial membrane, which was abolished by serosal ouabain. Decreases in the value of transmural potential difference were also produced by cooling, anoxia and serosal ouabain, but these were so small that concurrent changes in the membrane potential could be regarded as chiefly reflecting changes in the effective emf of the cell. Thus, an electrogenic Na+-K+ exchange pump located on the serosal membrane of the duodenal epithelial cells was shown to contribute significantly to the membrane potential under normal conditions (up to around -7 mV). The coupling ratio of Na+-efflux and K+-influx associated with this pump was estimated by the Mullins-Noda equation (1963) to be approximately 4:3 under the physiological steady-state conditions.

Animals

Effect of calcium on the membrane potential of Amphiuma red cells.

An increase in extracellular Ca concentration causes the membrane of giant red cells of the salamander, Amphiuma means, to undergo a marked, transient hyperpolarization. This hyperpolarization is caused by an increase in K permeability of the membrane as judged from the K sensitivity of the membrane potential and from the rate of K loss under influence of raised extracellular Ca concentration. At constant external pH, the induction of hyperpolarization by increased extracellular Ca has a relatively well-defined threshold concentration. Furthermore the phenomenon is of an "all or none" type with most of the cells having membrane potential values either in the normal range (about -15 mV) or in the range -40 to -70mV. Shortly after suspension in Ringer's with 15 mm Ca, most if not all of the individual cells are hyperpolarized. Upon continued exposure (5-20 min) to the higher Ca concentration the membrane potential returns to the normal value in a fashion compatible with an "all or none" response. The observed Ca effect is sensitive to the pH of the suspending medium. At pH 6.2 the response is absent whereas the hyperpolarization is markedly stronger at pH 8.2 than at PH 7.2. It is argued that a reliable transport number for K under influence of Ca cannot be estimated from the slope of membrane potential vs. log (extracellular K concentration). This is probably related to the fact that the membrane potentials of the cells in the population do not stay constant in time. The above phenomenon is compared with the Ca-induced K permeability in poisoned human red cells or red cell ghosts. It is important to note that the cells employed in the present study are neither poisoned nor mechanically disrupted. This study emphasizes that the role of Ca in regulating cell membrane permeability to K seems to be a general feature.

Animals

Membrane potential oscillations in molluscan "burster" neurones.

Membrane potential oscillations can be induced in molluscan neurones under a variety of artificial conditions. In the so-called 'burster' neurones oscillations are generated even in isolated cells. A likely mechanism for 'bursting' involves the following ionic currents: 1. A transient inward current carried by Na+ and Ca2+. This current is responsible for the upstroke of the action potentials. 2. A delayed outward current carried by K+. This current is voltage-sensitive and is responsible for the downstroke of the action potential during the early part of the burst. It becomes progressively inactivated during the burst. Its amplitude depends on the intracellular pH. 3. A rapidly developing outward current carried by K+ which is inactivated at potentials close to action potential threshold. This current tends to hold the membrane in the hyperpolarized state and is involved in spacing the action potentials. 4. A prolonged inward current which may not inactivate. It is probably carried by both Na+ and Ca2+. This current is responsible for the depolarizing phase of the burst but also contributes to the action potential. 5. A slowly developing outward current, carried by K+. This current appears as a result of a slow increase in intracellular ionized calcium and is responsible for the hyperpolarizing phase of the burst. Note that a transient increase in this current may also contribute to the falling phase of the action potential during the later stages of the burst. It is also sensitive to intracellular pH. One of the more significant features of this system of producing membrane potential oscillations is that the frequency of the bursts depends on the rate at which the intracellular ionized calcium returns to its resting level. This process depends on the metabolic state of the animal which can thereby exert a considerable influence on the electrical activity of burster neurones.

Animals

Changes in membrane potential during calcium ion influx and efflux across the mitochondrial membrane.

1. A depolarisation of the membrane of rat liver mitochondria, as measured with the safranine method, is seen during Ca2+ uptake. The depolarisation is followed by a slow repolarisation, the rate of which can be increased by the addition of EGTA or phosphate. 2. Plots relating the initial rate of calcium ion (Ca2+) uptake and the decrease in membrane potential (delta psi) to the Ca2+ concentration show a half-maximal change at less than 10 micron Ca2+ and a saturation above 20 micron Ca2+. 3. Plots relating the initial rate of Ca2+ uptake to delta psi are linear. 4. Addition of Ca2+ chelators, nitriloacetate or EGTA, to deenergized mitochondria equilibrated with Ca2+ causes a polarisation of the mitochondrial membrane due to a diffusion potential created by electrogenic Ca2+ efflux. 5. If the extent of the response induced by different nitriloacetate concentrations is plotted against the expected membrane potential a linear plot is obtained up to 70 mV with a slope corresponding to two-times the extent of the response induced by valinomycin in the presence of different potassium ion gradients. This suggests that the Ca2+ ion is transferred across the membrane with one net positive charge in present conditions.

Acetates

Erythrocyte membrane potentials determined by hydrogen ion distribution.

If the extracellular fluid is left unbuffered, dynamic membrane potential changes in the red blood cell may be determined from external pH readings. For some types of experiments it is necessary to accelerate H+ equilibration by adding minute amounts of hydrogen carriers. The method is independent of hematocrit over a wide range of membrane potential changes. Membrane potential jumps produced by permeability changes or by changes in ionic composition may be measured. The method provides a convenient means of measuring parameters of both the conductive and non-conductive anion pathways in the red cell.

Carbonyl Cyanide m-Chlorophenyl Hydrazone

Membrane potential of spinal motoneurons during natural sleep in cats.

The membrane potential of spinal motoneurons was recorded during wakefulness, NREM sleep, and REM sleep in minimally restrained, behaving cats. At the onset of sleep, the membrane potential generally increased in polarization in rough proportion to time spent asleep. During the postural atonia of REM sleep, the membrane potential of all motoneurons was tonically hyperpolarized. Antecedents of NREM sleep electromyographic suppressions, and REM sleep myoclonic twitches were seen as transient hyperpolarizations and depolarizations, respectively.

Animals