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The Golgi complex is present in every eukaryotic cell and functions in posttranslational modifications and sorting of proteins and lipids to post-Golgi destinations. Both functions require an acidic lumenal pH and transport of substrates into and by-products out of the Golgi lumen. Endogenous ion channels are expected to be important for these features, but none has been described. Ion channels from an enriched Golgi fraction cleared of transiting proteins were incorporated into planar lipid bilayers. Eighty percent of the single-channel recordings revealed the same anion channel. This channel has novel properties and has been named GOLAC (Golgi anion channel). The channel has six subconductance states with a maximum conductance of 130 pS, is open over 95% of the time, and is not voltage-gated. Significant for Golgi function, the channel conductance is increased by reduction of pH on the lumenal surface. This channel may serve two nonexclusive functions: providing counterions for the acidification of the Golgi lumen by the H(+)-ATPase and removal of inorganic phosphate generated by glycosylation and sulfation of proteins and lipids in the Golgi.

Individual ion channels are electrically isolated and studied in living cells with the tight patch voltage clamp method. Channels are identified, categorized, and sometimes named on the basis of the biophysical properties obtained with this method. Although it is usually presumed that these recordings are from native, undisturbed membrane, the physical basis of this technique is not well established. Observations that lipid blebs readily form when suction is applied to patch clamp electrodes suggest that many single channel recordings are from ion channels in these blebs.

1. Sodium channel current density was measured using the loose-patch voltage clamp technique. Innervated rat, mouse and snake muscle had the highest density of Na+ channels in the end-plate region. These high Na+ channel densities were maintained in denervated muscle. 2. Perijunctional membrane had a Na+ current density 5- to 10-fold greater than the density several hundred micrometres from the end-plate. In all muscles this concentration of channels near the end-plate persisted following denervation. 3. At the tendon Na+ current density fell to low values (approximately 1 mA/cm2). The decrease in density began about 300-500 microns from the tendon. This pattern was found in all snake twitch fibres and fast-twitch (EDL) rat and mouse muscle fibres. This reduction in channel density near the tendon was not affected by denervation. 4. Sodium channels in all regions of innervated rat and snake muscle fibres were highly sensitive to tetrodotoxin (TTX). Sodium channels in snake muscle remained sensitive to TTX after denervation. Sodium channels that are relatively resistant to TTX appeared in rat muscle after denervation. TTX-resistant channels were even more concentrated near the end-plate than were TTX-sensitive channels in innervated muscle. At the tendon TTX-resistant Na+ channel density decreased. 5. We conclude that although the nerve presumably directs the localization of Na+ channels during development, the ability to maintain this distribution and to control the distribution of newly appearing channels persists long after the nerve has been removed.

A vibrating probe was used to study a steady electric current generated by isolated, whole lumbrical muscles of the rat. Spatial mapping showed that current leaves the muscle in the synaptic region and re-enters in the flanking extrajunctional regions. The point of maximum outward current coincided precisely with the endplate region. As the probe was moved radially away from the endplate region, the current declined monotonically, and the results could be fit with a simple model. As the probe was moved axially away from the endplate region, the current declined and became inward over a distance of approximately 0.5 mm. The physiological mechanism by which the current is generated was also studied. alpha-Bungarotoxin and tetrodotoxin had no significant effect on the current, which suggests that acetylcholine channels and gated sodium channels are not involved in the generation of the current. Ouabain produced a slowly developing, partial inhibition of the current, reducing it by approximately 40% over a period of 30-40 min. Carbachol produced a large inward current at the endplate region. After the carbachol action was terminated with alpha-bungarotoxin, an outward current reappeared, and a transient "overshoot" developed. During the overshoot, which lasted approximately 30-40 min, the outward current was approximately doubled. This overshoot was completely abolished by ouabain. The overshoot is interpreted as reflecting the increased activity of electrogenic sodium pumping in the endplate region, caused by the influx of Na ions during carbachol application. Because of the very different actions of ouabain on the normal current and on the overshoot after carbachol application, we concluded that the normal outward current is not produced by electrogenic sodium pumping in the endplate region.

In an attempt to determine the mechanism by which rat skeletal muscle endplates generate a steady outward current, we measured the effects of several drugs (furosemide, bumetanide, 9-anthracene carboxylic acid [9-AC]) and changes in external ion concentration (Na+, K+, Cl-, Ba++) on resting membrane potential (Vm) and on the steady outward current. Each of the following treatments caused a 10-15-mV hyperpolarization of the membrane: replacement of extracellular Cl- with isethionate, addition of furosemide or bumetanide, and addition of 9-AC. These results suggest that Cl- is actively accumulated by the muscle fibers and that the equilibrium potential of Cl- is more positive than the membrane potential. Removal of external Na+ also caused a large hyperpolarization and is consistent with evidence in other tissues that active Cl- accumulation requires external Na+. The same treatments greatly reduced or abolished the steady outward current, with a time course that paralleled the changes in Vm. These results cannot be explained by a model in which the steady outward current is assumed to arise as a result of a nonuniform distribution of Na+ conductance, but they are consistent with models in which the steady current is produced by a nonuniform distribution of GCl or GK. Other treatments (Na+-free and K+-free solutions, and 50 microM BaCl2) caused a temporary reversal of the steady current. Parallel measurements of Vm suggested that in none of these cases did the electrochemical driving force for K+ change sign, which makes it unlikely that the steady current arises as a result of a nonuniform distribution of GK. All of the results, however, are consistent with a model in which the steady outward current arises as a result of a nonuniform distribution of Cl- conductance, with GCl lower near the endplate than in extrajunctional regions.

Injection of depolarizing current into vegetative cells of the water mold Blastocladiella emersonii elicits a regenerative response that has the electrical characteristics of an action potential. Once they have been taken past a threshold of about -40 mV, cells abruptly depolarize to +20 mV or above; after an interval ranging from several hundred milliseconds to a few seconds, the cells spontaneously return to their resting potential near -100 mV. When the action potential was analyzed with voltage-clamp recording, it proved to be biphasic. The initial phase reflects an influx of calcium ions through voltage-sensitive channels that also carry Sr2+ ions. The delayed, and more extended, phase of inward current results from the efflux of chloride and other anions. The anion channels are broadly selective, passing chloride, nitrate, phosphate, acetate, succinate and even PIPES. The anion channels open in response to the entry of calcium ions, but do not recognize Sr2+. Calcium channels, anion channels and calcium-specific receptors that link the two channels appear to form an ensemble whose physiological function is not known. Action potentials rarely occur spontaneously but can be elicited by osmotic downshock, suggesting that the ion channels may be involved in the regulation of turgor.

The loose patch voltage clamp has been used to map Na current density along the length of snake and rat skeletal muscle fibers. Na currents have been recorded from (a) endplate membrane exposed by removal of the nerve terminal, (b) membrane near the endplate, (c) extrajunctional membrane far from both the endplate and the tendon, and (d) membrane near the tendon. Na current densities recorded directly on the endplate were extremely high, exceeding 400 mA/cm2 in some patches. The membrane adjacent to the endplate has a current density about fivefold lower than that of the endplate, but about fivefold higher than the membrane 100-200 micron from the endplate. Small local variations in Na current density are recorded in extrajunctional membrane. A sharp decrease in Na current density occurs over the last few hundred micrometers from the tendon. We tested the ability of tetrodotoxin to block Na current in regions close to and far from the endplate and found no evidence for toxin-resistant channels in either region. There was also no obvious difference in the kinetics of Na current in the two regions. On the basis of the Na current densities measured with the loose patch clamp, we conclude that Na channels are abundant in the endplate and near-endplate membrane and are sparse close to the tendon. The current density at the endplate is two to three orders of magnitude higher than at the tendon.

Neuronal function depends crucially on the spatial segregation of specific membrane proteins, particularly the segregation associated with sites of synaptic contact. Understanding the factors governing this localization of proteins is a major goal of cellular neurobiology. A conspicuous example of synaptic specialization is the almost exclusive localization of vertebrate skeletal muscle acetylcholine (ACh) receptors to the subsynaptic membrane of the neuromuscular junction (for example, refs 1,2). The localization of other membrane proteins in skeletal muscle has been much less studied, but a knowledge of their distribution is crucial for understanding the factors governing regional specialization. We have explored the distribution in muscle of the voltage-gated Na channel responsible for the action potential using the loose patch-clamp technique, and have measured Na currents in 5-10 micron-diameter membrane patches as a function of distance from the end plate region of snake and rat muscle fibres. Here we report that the Na current density immediately adjacent to the endplate is 5-10-fold higher than at regions away from the endplate. The increased Na current density falls off rapidly with distance, reaching the background level 100-200 micron from the endplate. Although one might expect ACh receptors to be concentrated near the region of ACh release, such a concentration for Na channels, which propagate the impulse throughout the length of the cell, is surprising and suggests that factors similar to those responsible for concentrating ACh receptors at the endplate also operate to concentrate Na channels.

A previous paper reported that the water mold Blastocladiella emersonii generates a transcellular electrical current, such that positive charges enter the rhizoid and leave from the thallus (Stump et al., Proc. Natl. Acad. Sci. U.S.A. 77: 6673-6677, 1980). To begin to understand the genesis of this current we investigated ionic relationships in this organism by use of intracellular microelectrodes. In cells suspended in buffered CaCl2, the membrane potential could be accounted for as a K+ diffusion potential; no evidence for an electrogenic pump was obtained. Potassium ions diffuse outward by a pathway that also carries Rb+ and Ba2+, but excludes both smaller and larger ions (Li+, Na+, Cs+, Mg2+, Ca2+, and choline). Chloride and other anions make little contribution to the potential, but the presence of Ca2+ in the external medium is required for successful potential measurements. In growing cells, the internal K+ concentration is generally somewhat higher than would be expected if the K+ distribution were determined entirely by the membrane potential. Under certain conditions, net uptake of K+ against the electrochemical potential gradient was observed. We suggest that K+ is actively accumulated by a primary transport system that may exchange K+ for H+, and that K+ leaks passively outward through the K+ channel. The K+ circulation across the membrane amounts to about 2% of the K+ pool per min, or 4.5 microA/cm2 of surface area. We propose that this K+ circulation is one arm of the transcellular current, carrying positive charge out of the thallus.