Nature of the Schwann cell electrical potential. Effects of the external ionic concentrations and a cardiac glycoside

Electrical characteristics of the ionic psn-junction as a model of the resting axon membrane

As a model for the resting axon membrane, we propose the ionic psn-junction. Its electrical characteristics can be determined in close analogy to the corresponding electronic semiconductor junction. Using the "semianalytic approximation", we calculated the electrical capacity and the ionic currents. In contrast to the abrupt pn-junction, the electrical capacity of the psn-junction turns out to be practically voltage-independent, as it is observed for the squid axon membrane. The passive ionic fluxes for K(+), Na(+) and Cl(-), as the main contributions to the total charge flux, are calculated and compared with literature data on the ion fluxes through the resting squid axon membrane as measured by use of radioactive tracers. From this comparison, the ionic permeabilities can be evaluated and used to compute the resting membrane conductivity, which is found to be close to the experimental value. Further evidence in favor of the proposed asymmetrical membrane structure and possible ways of its test by the methods of protein chemistry are discussed.

Ionic currents in isolated and in situ squid Schwann cells

Ionic currents from Schwann cells isolated enzymatically from the giant axons of the squids Loligo forbesi, Loligo vulgaris and Loligo bleekeri were compared with those obtained in situ. Macroscopic and single channel ionic currents were recorded using whole-cell voltage and patch clamp. In the whole-cell configuration, depolarisation from negative holding potentials evoked two voltage-dependent currents, an inward current and a delayed outward current. The outward current resembled an outwardly rectifying K+ current and was activated at -40 mV after a latent period of 5-20 ms following a step depolarisation. The current was reduced by externally applied nifedipine, Co2+ or quinine, was not blocked by addition of apamin or charibdotoxin and was insensitive to externally applied L-glutamate or acetylcholine. The voltage-gated inward current was activated at -40 mV and was identified as an L-type calcium current sensitive to externally applied nifedipine. Schwann cells were impaled in situ in split-open axons and voltage clamped using discontinuous single electrode voltage clamp. Voltage dependent outward currents were recorded that were kinetically identical to those seen in isolated cells and that had similar current-voltage relations. Single channel currents were recorded from excised inside-out patches. A single channel type was observed with a reversal potential close to the equilibrium potential for K+ (E(K)) and was therefore identified as a K+ channel. The channel conductance was 43.6 pS when both internal and external solutions contained 150 mM K+. Activity was weakly dependent on membrane voltage but sensitive to the internal Ca2+ concentration. Activity was insensitive to externally or internally applied L-glutamate or acetylcholine. The results suggest that calcium channels and calcium-activated K+ channels play an important role in the generation of the squid Schwann cell membrane potential, which may be controlled by the resting intracellular Ca2+ level.

Electrochromic behaviour of carotenoid molecules in nerve cell membranes: a resonance Raman study

It was found that, following the depolarization of cell membranes of frog sciatic nerve, the 1521 and 1156 cm-1 resonance Raman (RR) bands of carotenoids showed an increase in intensity of 20%, 15% and 4% at excitation wavelengths of 488, 496.5 and 514.5 nm respectively. None of the bands revealed any change with excitation at 441.6, 457.9, 472.7 and 476.5 nm. These results can be explained by an electrochromic shift of the excitation profile of the RR bands by about 0.5 nm to the red. A dependence of the 1521 cm-1 band intensity on transmembrane potential was obtained. Under the effect of lanthanum ions, which are known to modify the surface charge of the membrane, the intensity of the Raman bands decreased by 15%-20% (excitation, 488.0 nm). The results obtained indicate that RR spectroscopy of carotenoids can be used to monitor changes in the transmembrane potential and surface charge of nerve cell membranes.

Ultrastructure and permeability of the Schwann cell layer surrounding the giant axon of the squid

The ultrastructure of the Schwann cell layer surrounding the giant axon of the squid Alloteuthis subulata is described, and the permeability of extracellular compartments assessed by exposure to electron-dense tracers. Morphometric analysis is used to deduce the number, size and shape of the Schwann cells, and the routes for ion flux across the Schwann cell layer. Axons (mean diameter 233 microns) were surrounded by a 1-2 microns thick layer of Schwann cells which were approximately 1 micron thick, approximately 70 microns long and approximately 23 microns wide. There were around 62,000 Schwann cells per cm2 axon surface. The outer (abaxonal) surface of the Schwann cells was invaginated, with evidence for a covering of fine Schwann cells processes; the inner (adaxonal) surface of the Schwann cells was less folded. The percentage area occupied by mesaxonal cleft openings to the axon and to the basal lamina was 0.02% and 1.09% respectively. A system of tubules, the glial tubular system, occupied 3.9% of the Schwann cell volume, and opened to both axonal and basal lamina surfaces, with more elaborate lattice-like clusters towards the basal side of the cell. Tubule openings accounted for 0.26% of the surface area facing the axon and 0.37% of the area facing the basal lamina (where there was greater clustering of openings). The electron dense tracers horseradish peroxidase, ionic lanthanum and tannic acid filled mesaxon clefts, glial tubular system and periaxonal space. If ion flux occurred via the mesaxonal clefts, a theoretical series resistance (Rsth) of > 20 omega cm2, would be predicted, whereas if it occurred via the tubular system, the figure would be < 2 omega cm2, closer to physiological estimates. The results presented show that the glial tubular system is likely to be the major route for ion flux into and across the Schwann cell layer, and for clearance of K+ from the periaxonal space during periods of axonal stimulation. The implications for K+ homeostasis in the axonal microenvironment are discussed.

Transfer of molecules from glia to axon in the squid may be mediated by glial vesicles

Although the transfer of glial proteins into the squid giant axon is well documented, the mechanism of the transfer remains unknown. We examined the possibility that the transfer involved membrane-bound vesicles, by taking advantage of the fact that the fluorescent compound, 3,6-acridinediamine, N,N,N,',N'-tetramethylmonohydride [acridine orange (AO)], rapidly and selectively stains vesicular structures in glial cells surrounding the giant axon. We labeled cleaned axons (1-3 cm long) by incubation for 1 min in filtered seawater (FSW) containing AO. Because the AO was concentrated in glial vesicular organelles, these fluoresced bright orange when the axon was examined by epifluorescence microscopy. To look for vesicle transfer, axoplasm was extruded from such AO-treated axons at various times after labeling. During the initial 15 min, an increasing number of fluorescent vesicles were observed. No further increases were observed between 15 and 60 min post AO. The transfer of the fluorescent vesicles into the axoplasm seemed to be energy dependent, as it was inhibited in axons treated with 2 mM KCN. These results suggest that a special mode of exchange exists between the adaxonal glia and the axon, perhaps involving phagocytosis by the axon of small portions of the glial cells.

Studies of axon-glial cell interactions and periaxonal K- homeostasis--I. The influence of Na+, K+, Cl- and cholinergic agents on the membrane potential of the adaxonal glia of the crayfish medial giant axon

The ionic basis for the low (-40 mV) resting membrane potential of glial cells surrounding the giant axons of the crayfish and their hyperpolarization by cholinergic agents (to -55 mV) was studied using standard electrophysiological techniques, ionic substitutions and pharmacological agents. The resting membrane potential of the glial cell was depolarized by increasing [K+]o, but the response was not Nernstian. Na+ depletion caused a small depolarization of the glial resting membrane potential, whereas Cl- depletion resulted in a hyperpolarization comparable to that seen with carbachol at various [K+]o. Both furosemide (1 mM) and bumetanide (0.1 mM) produced an 8-10 mV hyperpolarization as compared to 15-17 mV seen with Cl- depletion or carbachol. Carbachol has no further effect on the potential following furosemide treatment or Cl- depletion. After carbachol administration or Cl- depletion the resting membrane potential of the glial cell responded to [K+]o in a more Nernstian manner. The data indicate that the low resting membrane potential of glial cells is due to a combination of a low [K+]i and an outwardly-directed (depolarizing) Cl- electrochemical gradient. Carbachol acts to decrease Cl- conductance, resulting in the hyperpolarization of the glial cell membrane and a decrease in the outwardly-directed K+ electrochemical gradient by approximately two-thirds. We hypothesize that this mechanism for modulation of the glial cell membrane potential and the K+ electrochemical gradient serves to enhance the uptake of K+ by the glial cell transport system.

Freeze-fracture studies on the giant axon and ensheathing Schwann cells of the squid

The giant axons and encompassing sheaths from the stellar nerves of the squids Sepioteuthis sepioidea and Loligo forbesi have been analysed by freeze-fracture. The axolemma exhibits many intramembranous particles (IMPs) that fracture onto the cytoplasmic membrane half-leaflet (P-face); the larger IMPs may be aggregated into clusters. Axoplasmic subsurface cisternae are found beneath this membrane. Clustered or aligned arrays of P-face IMPs are also found on the membranes of the Schwann cells that intimately encapsulate the giant axons as well as 'capitate' projections of Schwann cells into the axons. When adjacent Schwann cells abut directly against one another, aligned E-face IMPs are found along the fracture plane of the upturning membranes. These E-face alignments of IMPs have complementary furrows on the Schwann cell membranes which exhibit no complementary structure on the axolemma as they represent the clefts between adjacent glial cells. The other Schwann cell membranes exhibit P-face dimples and E-face (extracellular membrane half-leaflet) protuberances which may reflect endo- or exocytotic activity; alternatively they may represent caveolae. Comparable structures are occasionally observed at axo-glial interfaces. However, those in the Schwann cell membrane could be part of the transverse tubular lattice system which also exists in adaxonal glia. Beyond the Schwann cells, layers of endoneurial cells (fibrocytes) are interleaved by collagen-filled spaces. These cells exhibit extensive cross-fractured intracellular invaginations as well as inpushings of the extracellular matrix material. Their membranes exhibit a large number of IMPs.

Sodium transport in astrocytes

Sodium transport in astrocytes in homogeneous primary cultures from mouse brain cortex were investigated with radiotracer (22Na) and electrophysiological methods. The equilibrated Na+ content was 190 nmol X mg-1 protein and the influx and efflux rates were identical at about 560 nmol X mg-1 X min-1. No significant change was observed in Na+ efflux or influx when external K+ was raised from 5.4 to 12 or 54 mM, but the Na+ content decreased. Intracellular Na+ loading, evoked by previous exposure to ice-cold K+-free medium, double the Na+ efflux. Ouabain, a Na+-K+ exchange inhibitor, exerted a small, nonsignificant inhibition of Na+ efflux at both 5.4 and 12 mM K+ and caused a large increase in Na+ content. At 5.4 mM K+, amiloride, a Na+-H+ exchange inhibitor, decreased both influx and efflux of Na+ and caused an increase in Na+ content. Furosemide, an inhibitor of a cation-Cl- carrier, decreased both content and influx of Na+ slightly but had no significant effect on Na+ efflux. The effects of amiloride or furosemide on Na+ influx were abolished at elevated (12 and 54 mM) K+. Attempts to stimulate the Na+-K+ pump with elevated external K+ or internal Na+ produced no electrogenic component of the membrane potential, probably owing to the high K+ permeability. Based on the present results and earlier experiments on K+ influx, it is concluded that 1) the Na+-K+ pump of astrocytes under normal conditions transports more K+ than Na+; 2) intracellular Na+ loading increases Na+ efflux; 3) some Na+-H+ exchange and cotransport of Na+ and Cl- seem to occur at 5.4 mM K+; and 4) neither of the latter two transport mechanisms is enhanced at elevated K+ concentrations.

Electrophysiological and pharmacological properties of glial cells associated with the medial giant axon of the crayfish with implications four neuron-glial cell interactions

Schwann-like glial cells surrounding the medial giant axon of the crayfish (Procambarus clarkii) were impaled with glass microelectrodes to study their responses to cholinomimetics, cholinergic receptor blockers and ouabain. Axon electrical properties were simultaneously monitored. Glial cells have a low membrane potential compared to the axon; -42 mV and -85 mV, respectively. Acetylcholine, carbachol and nicotine hyperpolarized the glial cells but did not affect the axon steady-state or active membrane potentials. The action of the cholinergics was completely blocked by d-tubocurarine and alpha-bungarotoxin. Ouabain hyperpolarized the glial cell but depolarized the axon. Tubocurarine blocked the ouabain hyperpolarization but not the delayed depolarization of the glia cell or the axon. It is concluded that ouabain causes the release of acetylcholine from the glial cell-axon preparation, inducing the glial hyperpolarization. Studies of the axon-glial cell interaction suggest that a function of the glial cell is to actively modulate the periaxonal potassium concentration on a signal from the axon. Periaxonal potassium can strongly affect axon membrane potential through electrogenic Na transport, modifying axon signalling properties.

Structural complexes in the squid giant axon membrane sensitive to ionic concentrations and cardiac glycosides

Giant nerve fibers of squid Sepioteuthis sepioidea were incubated for 10 min in artificial sea water (ASW) under control conditions, in the absence of various ions, and in the presence of cardiac glycosides. The nerve fibers were fixed in OsO4 and embedded in Epon, and structural complexes along the axolemma were studied.

Grayanotoxin, veratrine, and tetrodotoxin-sensitive sodium pathways in the Schwann cell membrane of squid nerve fibers

The actions of grayanotoxin I, veratrine, and tetrodotoxin on the membrane potential of the Schwann cell were studied in the giant nerve fiber of the squid Sepioteuthis sepioidea. Schwann cells of intact nerve fibers and Schwann cells attached to axons cut lengthwise over several millimeters were utilized. The axon membrane potential in the intact nerve fibers was also monitored. The effects of grayanotoxin I and veratrine on the membrane potential of the Schwann cell were found to be similar to those they produce on the resting membrane potential of the giant axon. Thus, grayanotoxin I (1-30 muM) and veratrine (5-50 mug-jl-1), externally applied to the intact nerve fiber or to axon-free nerve fiber sheaths, produce a Schwann cell depolarization which can be reversed by decreasing the external sodium concentration or by external application of tetrodotoxin. The magnitude of these membrane potential changes is related to the concentrations of the drugs in the external medium. These results indicate the existence of sodium pathways in the electrically unexcitable Schwann cell membrane of S. sepioidea, which can be opened up by grayanotoxin I and veratrine, and afterwards are blocked by tetrodotoxin. The sodium pathways of the Schwann cell membrane appear to be different from those of the axolemma which show a voltage-dependent conductance.

Neurotransmission and glial cells: a functional relationship?

The investigations reported here demonstrate high affinity transport systems localized in glial cells which appear to be specific for amino acid neurotransmitter candidates. Data on uptake of gamma-aminobutyric acid (GABA), glutamate, glycine, and taurine, show transport systems with KT'S in the range of 10(-5) M. In addition, the distribution of the glial transport system for glycine is shown to parallel the presumed distribution of glycine as an inhibitory neurotransmitter. Results of these studies also suggest that transport studies on brain homogenates or synaptosomal preparations do not serve to localize these functions to synaptic elements as is widely believed. This report shows that glia can form vesicles during homogenization which band which synaptosomes in density gradients, and retain transport activity. Glia also may contribute to the release of neurotransmitters via control of the extracellular Ca++ concentration. This is shown by the ability of GABA in the extracellular media to cause release of Ca++ by glia.

Relationship between membrane potential and external potassium in human glioblastoma cells in tissue culture

Cells from a human glioblastoma (TC 526) maintained in tissue culture for ten years had a mean membrane potential of 27 +/- 0.9 mV at an external potassium concentration [Ko] of 5.3 mM. When [Ko] was varied between 2.5 and 5.3 mM, membrane potential changes were close to those predicted by the Nernst equation. At higher [Ko], the Nernstian slope was approached only in the presence of 10(-5) M ouabain, which did not affect membrane potential at a [Ko] of 5.3 mM. An electrogenic sodium pump activated by high [Ko] could explain these findings; such a mechanism has been demonstrated in other tissues.

Effects of acetylcholine and carbamylcholine on the axon and Schwann cell electrical potentials in the squid nerve fibre

1. The effect of acetylcholine and carbamylcholine on the axon and Schwann cell membrane potential have been studied in the giant nerve fibre of the squid. The addition of carbamylcholine (10(-6)M) to the external sea-water medium has no appreciable effects on the resting and action potentials of the axon. However, it induces a long-lasting hyperpolarization in the surrounding Schwann cells of the unstimulated intact or slit nerve fibres which is completely blocked by D-tubocurarine (10(-9)M). Eserine (10(-9)M) prolongs the Schwann cell hyperpolarizations induced by a 1 min exposure of the unstimulated nerve fibres to acetylcholine (10(-7)M).2. The addition of carbamylcholine (10(-6)M) to the external medium increases the relative permeability of the Schwann cell membrane to the potassium ion in slit nerve fibres. Yet, a hundredfold reduction in external sodium concentration has no appreciable effect on the hyperpolarization of the Schwann cells of the slit nerve fibre under similar conditions.3. Tetrodotoxin at a concentration of 5 x 10(-8)M has no appreciable effects on either the Schwann cell electrical potential or on the hyperpolarizing action of carbamylcholine on the Schwann cells of the unstimulated intact nerve fibres.4. These findings indicate the presence of acetylcholine receptors in the plasma membrane of the Schwann cell in these nerve fibres and give further support to the hypothesis on the role of the cholinergic system in the genesis of the long-lasting Schwann cell hyperpolarizations caused by the conduction of nerve impulse trains by the axon.

Axon-Schwann cell interaction in the squid nerve fibre

The electrical properties of Schwann cells and the effects of neuronal impulses on their membrane potential have been studied in the giant nerve fibre of the squid.1. The behaviour of the Schwann cell membrane to current injection into the cell was ohmic. No impulse-like responses were observed with displacements of 35 mV in the membrane potential. The resistance of the Schwann cell membrane was found to be approximately 10(3) Omega cm(2).2. A long-lasting hyperpolarization is observed in the Schwann cells following the conduction of impulse trains by the axon. Whereas the propagation of a single impulse had little effect, prolonged stimulation of the fibre at 250 impulses/sec was followed by a hyperpolarization of the Schwann cell that gradually declined over a period of several minutes.3. The prolonged effects of nerve impulse trains on the Schwann cell were similar to those produced by depolarizing current pulses applied to the axon by the voltage-clamp technique. Thus, a series of depolarizing pulses in the axon was followed by a long-lasting hyperpolarization of the Schwann cells. In contrast, the application of a series of hyperpolarizing 100 mV pulses at a frequency of 1/sec had no apparent effects.4. Changes in the external potassium concentration did not reproduce the long-lasting effects of nerve excitation.5. The hyperpolarizing effects of impulse trains were abolished by the incubation of the nerve fibre in a sea-water solution containing trypsin.6. These findings are discussed in relation to the possible mechanisms that might be responsible for the long-lasting hyperpolarizations of the Schwann cells.

Some physiological properties of identified mammalian neuroglial cells

Mammalian glial cells were identified and studied in the optic nerves of anaesthetized rats. Cells with membrane potentials of 77-85 mV were located in the optic nerve with capillary micropipettes. These were shown to be neuroglia by iontophoretic injection of a fluorescent dye through the recording electrode, followed by histological verification of the location of the dye. No distinction was made between astroglia and oligodendroglia. Neuroglial cells gave no impulse activity. Their membrane potential was studied in isolated optic nerves by varying the ionic composition of the bathing fluid. The glial membrane potential depends predominantly on a transmembrane gradient of potassium ions.

Adenosine triphosphatase activity in the membranes of the squid nerve fiber

This investigation deals with the localization of sites of ATPase activity, especially of transport ATPase, in nerve fibers of the squid Doryteuthis plei, at the subcellular level. Splitting of ATP liberates inorganic phosphate which reacts with lead to form a precipitate in the tissue. The reaction was made on nerve fibers fixed with glutaraldehyde. Frozen slices were incubated in Wachstein-Meisel medium containing ATP and Pb(NO(3))(2). Deposits of reaction product were found in the axolemma (towards its axoplasmic side), Schwann cell membranes (mainly at the channels crossing the layer), and mitochondria. Control experiments revealed that no deposits were observed in nerve fibers fixed in osmium tetroxide prior to incubation in the medium containing ATP, or in nerve fibers incubated without substrate or with adenosine monophosphate, adenosine diphosphate, glycerophosphate, or guanosine triphosphate as substrate. For evaluation of transport ATPase activity, these findings were compared with results obtained with nerve fibers treated with G-strophanthin or K-strophanthoside before or after glutaraldehyde fixation. The cardiac glycosides produced a disappearance or diminution of the deposits. The largest inhibitory effect was observed in the axolemma. The findings indicate that the highest ATPase activity is localized in the axolemma and may be due primarily to transport ATPase.