Action potentials without contraction in frog skeletal muscle fibers with disrupted transverse tubules.

Action potentials, with no accompanying contraction, were recorded from muscle fibers in which the transverse tubular system had been disrupted. The results show that action potentials require an intact transverse tubular system to cause contraction. Furthermore, both the after-depolarization following a single action potential and the slower, late afterpotential following a train of action potentials were absent in this preparation. Therefore, both phenomena must normally involve the transverse tubular system.

Frog skeletal muscle fibers: changes in electrical properties after disruption of transverse tubular system.

In muscle fibers which have been exposed for 1 hour to a Ringer solution containing 400 millimolar glycerol and then returned to plain Ringer solution, the transverse tubular system is disrupted. At the same time the membrane capacitance is markedly reduced and hyperpolarizing current pulses no longer produce a slow, progressive increase in potential (creep). The large capacitance of muscle and the phenomenon of "creep" must both depend on an intact transverse tubular system.

Synaptic current at the squid giant synapse.

Transmission in the giant synapse of squid was studied by measuring synaptic currents in the voltage-clamped postsynaptic giant axon. These currents varied linearly with the axon's membrane potential, and showed an intercept on the voltage axis at, or near, the sodium equilibrium potential. The intercept shifted in seawater containing less sodium by even more than the shift in the sodium equilibrium potential. It is concluded that the transmitter at this synapse causes a significant change in the sodium conductance only.

Gating currents associated with sodium and calcium currents in an Aplysia neuron.

In a voltage-clamped aplysia neuron (R15), depolarization beyond -30 millivolts produces an inward sodium current. Depolarization beyond -10 millivolts produces an additional inward calcium current with slower kinetics than the sodium current. When these ionic currents have been suppressed and capacitive currents subtracted out, a small outward displacement current can be seen with depolarizations beyond -30 millivolts. An additional, slower displacement current is seen with depolarizations beyond -10 millivolts. The currents have an exponential decay with an increase in rate per 10 degrees C increase in temperature of about 3 and are thought to be sodium and calcium gating currents.

Activation and modulation of neuronal K+ channels by GABA.

Although the concept of GABAB receptors was introduced only ten years ago, several actions of GABAB agonists are already well established. They cause depression of transmitter release, a decrease in voltage-dependent Ca2+ conductance and an increase in K+ conductance. It has recently been reported that GABA also changes the voltage dependence of the transient ('A' type) K+ channel. Depression of transmitter release by GABAB agonists may be caused by a decrease in Ca2+ conductance, an increase in K+ conductance or a modulation of A channels in presynaptic nerve terminals. Slow IPSPs in some neurons are generated by an increase in K+ conductance that can be blocked by GABAB antagonists and pertussis toxin. K+ channels of variable amplitude that are blocked by pertussis toxin are activated by GABAB agonists in cultured hippocampal neurons. Since arachidonic acid activates similar channels in excised patches of membrane, it may form part of a normal second messenger system linking GABAB receptors to K+ channels.

Capacitance of the surface and transverse tubular membrane of frog sartorius muscle fibers.

The passive electrical properties of glycerol-treated muscle fibers, which have virtually no transverse tubules, were determined. Current was passed through one intracellular microelectrode and the time course and spatial distribution of the resulting potential displacement measured with another. The results were analyzed by using conventional cable equations. The membrane resistance of fibers without tubules was 3759 +/- 331 ohm-cm(2) and the internal resistivity 192 ohm-cm. Both these figures are essentially the same as those found in normal muscle fibers. The capacitance of the fibers without tubules is strikingly smaller than normal, being 2.24 +/- 0.14 microF/cm(2). Measurements were also made of the passive electrical properties of fibers in a Ringer solution containing 400 mM glycerol (which is used in the preparation of glycerol-treated fibers). The membrane resistance and capacitance are essentially normal, but the internal resistivity is somewhat reduced. These results show that glycerol in this concentration does not directly affect the membrane capacitance. Thus, the figure for the capacitance of glycerol-treated fibers, which agrees well with previous estimates made by different techniques, represents the capacitance of the outer membrane of the fiber. Estimates of the capacitance per unit area of the tubular membrane are made and the significance of the difference between the figures for the capacitance of the surface and tubular membrane is discussed.

Ionic conductances of the surface and transverse tubular membranes of frog sartorius fibers.

The resting ionic conductances of frog sartorius muscle fibers have been determined in a variety of conditions in order to measure the potassium conductance of the tubular and surface membranes (gK(t) and gK(s)) and the chloride conductance of the tubular and surface membranes (gCl(t) and gCl(s)). In both normal fibers and fibers without tubules, measurements of input resistance and diameter were made at normal pH and at low pH when the chloride conductance was very small. These measurements permitted the separation of the ionic conductances: gCl(s) = 219 micromhos/cm(2); gCl(t) = 0 micromhos/cm(2); gK(s) = 28 micromhos/cm(2); gK(t) = 55 micromhos/cm(2). Possible sources of systematic error are discussed and a statistical analysis of the effects of random error is presented. The implications of the nonuniformity of membrane properties are discussed along with possible anatomical explanations.

Action potentials, afterpotentials, and excitation-contraction coupling in frog sartorius fibers without transverse tubules.

In frog sartorius muscle fibers in which the transverse tubular system has been disrupted by treatment with glycerol, action potentials which are unaccompanied by twitches can be recorded. These action potentials appear to be the same as those recorded in normal fibers except that the early afterpotential usually consists of a small hyperpolarization of short duration. After a train of action potentials no late afterpotential is seen even when the membrane potential is changed from the resting level. In fibers without transverse tubules hyperpolarizing currents do not produce a creep in potential. The interruption of excitation-contraction coupling, the changes in the afterpotentials, and the disappearance of creep are all attributed to the lack of a transverse tubular system.

Potassium current activated by depolarization of dissociated neurons from adult guinea pig hippocampus.

Currents were generated by depolarizing pulses in voltage-clamped, dissociated neurons from the CA1 region of adult guinea pig hippocampus in solutions containing 1 microm tetrodotoxin. When the extracellular potassium concentration was 100 mM, the currents reversed at -8.1 +/- 1.6 mV (n = 5), close to the calculated potassium equilibrium potential of -7 mV. The currents were depressed by 30 mM tetraethylammonium in the extracellular solution but were unaffected by 4-aminopyridine at concentrations of 0.5 or 1 mM. It was concluded that the currents were depolarization-activated potassium currents. Instantaneous current-voltage curves were nonlinear but could be fitted by a Goldman-Hodgkin-Katz equation with PNa/PK = 0.04. Conductance-voltage curves could be described by a Boltzmann-type equation: the average maximum conductance was 65.2 +/- 15.7 nS (n = 9) and the potential at which gK was half-maximal was -4.8 +/- 3.9 mV (mean +/- 1 SEM, n = 10). The relationship between the null potential and the extracellular potassium concentration was nonlinear and could be fitted by a Goldman-Hodgkin-Katz equation with PNa/PK = 0.04. The rising phase of potassium currents and the decay of tail currents could be fitted with exponentials with single time constants that varied with membrane potential. Potassium currents inactivated to a steady level with a time constant of approximately 450 ms that did not vary with potential. The currents were depressed by substituting cobalt or cadmium for extracellular calcium but similar effects were not obtained by substituting magnesium for calcium.

The sodium current underlying action potentials in guinea pig hippocampal CA1 neurons.

Neurons were acutely dissociated from the CA1 region of hippocampal slices from guinea pigs. Whole-cell recording techniques were used to record and control membrane potential. When the electrode contained KF, the average resting potential was about -40 mV and action potentials in cells at -80 mV (current-clamped) had an amplitude greater than 100 mV. Cells were voltage-clamped at 22-24 degrees C with electrodes containing CsF. Inward currents generated with depolarizing voltage pulses reversed close to the sodium equilibrium potential and could be completely blocked with tetrodotoxin (1 microM). The amplitude of these sodium currents was maximal at about -20 mV and the amplitude of the tail currents was linear with potential, which indicates that the channels were ohmic. The sodium conductance increased with depolarization in a range from -60 to 0 mV with an average half-maximum at about -40 mV. The decay of the currents was not exponential at potentials more positive than -20 mV. The time to peak and half-decay time of the currents varied with potential and temperature. Half of the channels were inactivated at a potential of -75 mV and inactivation was essentially complete at -40 to -30 mV. Recovery from inactivation was not exponential and the rate varied with potential. At lower temperatures, the amplitude of sodium currents decreased, their time course became longer, and half-maximal inactivation shifted to more negative potentials. In a small fraction of cells studied, sodium currents were much more rapid but the voltage dependence of activation and inactivation was very similar.

Effects of ammonium ions on endplate channels.

Miniature endplate currents, recorded from voltage-clamped toad sartorius muscle fibers in solutions containing ammonium ions substituted for sodium ions, were increased in amplitude and decayed exponentially with a slower time constant than in control (Na) solution. The peak conductance of miniature endplate currents was also greater in ammonium solutions. The acetylcholine null potential was -2.8 +/- 0.8 mV in control solution, and shifted to 0.9 +/- 1.6 mV in solutions in which NH4Cl replaced half the NaCl. In solutions containing NH4Cl substituted for all the NaCl, the null potential was 6.5 +/- 1.3 mV. Single channel conductance and average channel lifetime were both increased in solutions containing ammonium ions. The exponential relationship between the time constant of decay of miniature endplate currents or channel lifetime and membrane potential was unchanged in ammonium solutions. A slight but consistent increase in peak conductance during miniature endplate currents and single channel conductance was seen as membrane potential became more positive (depolarized) in both control and ammonium solutions. Net charge transfer was greater in ammonium solutions than in control solution, whether measured during a miniature endplate current or through a single channel. The results presented here are consistent with an endplate channel model containing high field strength, neutral sites.

A voltage-dependent persistent sodium current in mammalian hippocampal neurons.

Currents generated by depolarizing voltage pulses were recorded in neurons from the pyramidal cell layer of the CA1 region of rat or guinea pig hippocampus with single electrode voltage-clamp or tight-seal whole-cell voltage-clamp techniques. In neurons in situ in slices, and in dissociated neurons, subtraction of currents generated by identical depolarizing voltage pulses before and after exposure to tetrodotoxin revealed a small, persistent current after the transient current. These currents could also be recorded directly in dissociated neurons in which other ionic currents were effectively suppressed. It was concluded that the persistent current was carried by sodium ions because it was blocked by TTX, decreased in amplitude when extracellular sodium concentration was reduced, and was not blocked by cadmium. The amplitude of the persistent sodium current varied with clamp potential, being detectable at potentials as negative as -70 mV and reaching a maximum at approximately -40 mV. The maximum amplitude at -40 mV in 21 cells in slices was -0.34 +/- 0.05 nA (mean +/- 1 SEM) and -0.21 +/- 0.05 nA in 10 dissociated neurons. Persistent sodium conductance increased sigmoidally with a potential between -70 and -30 mV and could be fitted with the Boltzmann equation, g = gmax/(1 + exp[(V' - V)/k)]). The average gmax was 7.8 +/- 1.1 nS in the 21 neurons in slices and 4.4 +/- 1.6 nS in the 10 dissociated cells that had lost their processes indicating that the channels responsible are probably most densely aggregated on or close to the soma. The half-maximum conductance occurred close to -50 mV, both in neurons in slices and in dissociated neurons, and the slope factor (k) was 5-9 mV. The persistent sodium current was much more resistant to inactivation by depolarization than the transient current and could be recorded at greater than 50% of its normal amplitude when the transient current was completely inactivated. Because the persistent sodium current activates at potentials close to the resting membrane potential and is very resistant to inactivation, it probably plays an important role in the repetitive firing of action potentials caused by prolonged depolarizations such as those that occur during barrages of synaptic inputs into these cells.

Cation-selective ion channels formed by p7 of hepatitis C virus are blocked by hexamethylene amiloride.

A 63 residue peptide, p7, encoded by hepatitis C virus was synthesised and tested for ion channel activity in lipid bilayer membranes. Ion channels formed by p7 had a variable conductance: some channels had conductances as low as 14 pS. The reversal potential of currents flowing through the channels formed by p7 showed that they were permeable to potassium and sodium ions and less permeable to calcium ions. Addition of Ca(2+) to solutions made channels formed by p7 less potassium- or sodium-selective. Hexamethylene amiloride, a drug previously shown to block ion channels formed by Vpu encoded by HIV-1, blocked channels formed by p7. In view of the increasing number of peptides encoded by viruses that have been shown to form ion channels, it is suggested that ion channels may play an important role in the life cycle of many viruses and that drugs that block these channels may prove to be useful antiviral agents.

Muscarinic acetylcholine receptor produced in recombinant baculovirus infected Sf9 insect cells couples with endogenous G-proteins to activate ion channels.

Following the infection of insect ovarian cells (Sf9) with recombinant bearing the cDNA coding for the rat muscarinic acetylcholine (ACh) receptor subtype m3, ionic flux across the membrane in response to the application of ACh was examined electrophysiologically. We show that ACh activates potassium currents. The response is abolished when cells are treated with pertussis toxin. No ACh-induced currents are observed from uninfected cells or cells infected with virus which do not contain the cDNA coding for ACh receptors in its genome. The characteristics of single channel currents show time-dependent changes following the application of ACh. Initially, ACh activates brief channel currents with a conductance of about 5 pS. The conductance level of channels gradually increases in steps to 10 pS and then to 20 pS and 40 pS. At the same time, channel open probability also increases. Thereafter, additional channels appear, opening and closing independently of, or at times in synchrony with, the original channel.

Influence of membrane potential on conductance sublevels of chloride channels activated by GABA.

Single-channel chloride currents activated by 0.5 microM GABA were recorded in cell-attached and inside-out membrane patches from rat cultured hippocampal neurons. The currents displayed multiple conductance states and outward rectification. The number and amplitude of conductance levels were determined over a range of potentials by using digital signal-processing techniques. It was found that, except for a level close to zero, subconductance levels were regularly spaced. There were fewer sublevels at hyperpolarized than at depolarized potentials, and the spacing between levels varied linearly with potential giving an incremental conductance of 8-10 pS that was independent of membrane potential. Outward rectification is related to the change in the number of conductance levels with potential. One hypothesis that is consistent with these observations is that a channel is composed of a number of synchronized, non-rectifying, conducting pores, and that the number of pores activated changes with membrane potential.

Inactivation-resistant channels underlying the persistent sodium current in rat ventricular myocytes.

Single-channel sodium currents that could be blocked with TTX were elicited by depolarizing voltage pulses in either cell-attached or inside-out patches from rat ventricular myocytes. A transient burst of channels was followed by late-opening (persistent) channels with low open probability. Conditioning depolarizing pre-pulses that inactivated transient channels and 'chattering' late-opening channels had no effect on persistent channels. The open probability of persistent channels reached a maximum at more negative potentials than transient channels. Between -70 mV and -40 mV, the average open time of persistent channels increased, whereas the average open time of transient channels did not change significantly, so the open times of the two channels diverged as the potential became more positive. The conductance of transient and persistent channels was similar, and the conductance of both kinds of channel increased at more depolarized potentials.

GABA-induced potassium channels in cultured neurons.

When gamma-aminobutyric acid (GABA) or baclofen were applied to cultured rat hippocampal neurons, single-channel potassium currents appeared after a delay of 30 s or more in patches of membrane on the cell surface isolated from the agonists by the recording pipette. The appearance of currents in patches not exposed to agonist, the delay in their appearance and the suppression of currents in cells pre-incubated with pertussis toxin indicate the involvement of an intracellular second messenger system. The channels were associated with a GABAB receptor rather than a GABAA receptor as they were blocked by baclofen, a GABAB antagonist, but were not affected by bicuculline, a GABAA antagonist. A feature of the single channel currents was their variable amplitude: they had a maximum conductance of ca. 70 pS and displayed many lower conductance states that were integral multiples of 5-6 pS. In several cells exposed to GABA or baclofen, first small currents and then progressively larger currents appeared: current amplitude was a multiple of an elementary current. It is suggested that binding of GABA to GABAB receptors activates a second messenger system causing opening of oligomeric potassium channels.

Coupled potassium channels induced by arachidonic acid in cultured neurons.

Exposure of the inside surface of patches of membrane excised from cultured rat hippocampal neurons to arachidonic acid (10-100 microM) caused the appearance of potassium currents of variable amplitude similar to those activated by GABA or baclofen in cell-attached patches. The amplitude of single-channel currents increased with time after exposure to 20 or 50 microM arachidonic acid and also increased when arachidonic acid concentration was increased from 20 to 50 or 100 microM. Current-amplitude probability histograms had peaks at integral multiples of an 'elementary' current. It is proposed that arachidonic acid or its metabolites cause synchronous opening and closing of coupled conducting units (co-channels) in cell membranes.

A combination of human alpha 1 and beta 1 subunits is required for formation of detectable GABA-activated chloride channels in Sf9 cells.

The baculovirus expression system was used to produce alpha 1 and beta 1 subunits of the human GABAA receptor in Sf9 cells. In cells infected with both alpha 1 and beta 1 recombinant viruses, GABA elicited an outwardly rectifying chloride current that was blocked by bicuculline and potentiated by pentobarbitone. GABA did not produce detectable currents in cells infected with either alpha 1 or beta 1 recombinant viruses alone. In these cells, and in control (non-infected) Sf9 cells, pentobarbitone depressed the leakage current (Ki = 55 microM). Fluorescently labelled monoclonal antibodies to the alpha 1 subunit showed greater amounts of the alpha 1 subunit in cells infected with only the alpha 1 recombinant virus than in cells co-infected with the alpha 1 and beta 1 recombinant viruses. Fluorescence of the plasma membrane was seen in cells co-infected with the alpha 1 and beta 1 recombinant viruses, but was absent in cells infected with only the alpha 1 recombinant virus. It was concluded that the alpha 1 subunit normally interacts with the beta 1 subunit to be transported to the plasma membrane in Sf9 cells.

Postsynaptic effects of some central stimulants at the neuromuscular junction.

1 Miniature endplate currents (m.e.p.cs) were recorded with extracellular electrodes from sartorius muscles of toads. 2 Central excitant analogues of amylobarbitone (3M2B) and halothane (DBE) decreased the amplitude and time constant of decay of m.e.p.cs and hence reduced the amplitude of miniature endplate potentials. The decay remained exponential with single time constant. 3 A central excitant analogue of ether (indoklon) reduced the amplitude of m.e.p.cs and made their decay biphasic. The decay could be fitted by the sum of two exponentials. 4 Bemegride, a central excitant, prolonged m.e.p.cs. Their decay remained exponential with single time constant. The effect was not due to inhibition of acetylcholinesterase. 5 All of the drugs tested, including amylobarbitone, reduced the temperature-sensitivity of the decay of m.e.p.cs. 6 The biphasic decay of m.e.p.cs caused by indoklon could not be explained simply by supposing that the drug blocked open endplate channels unless it was assumed that the normal rate of channel closing also increased and became much less temperature-sensitive than normal.