Patch and whole cell calcium currents recorded simultaneously in snail neurons

The flow of Ca ions through single Ca channels has been examined. The gigaseal method was used on identifiable snail neurons that were voltage clamped using a two-microelectrode voltage clamp method. Average Ca patch currents and whole cell currents have similar time courses. They are affected similarly by changes in temperature. The differences in amplitude and inactivation between Ba and Ca whole cell currents were present in the patch records. The stationary noise spectra recorded from ensembles of multichannel patches have two components with fast and slow time constants equivalent to two components in the whole cell tail current relaxations. Elementary current amplitudes measured from the variance-mean relationship and from noise spectra gave values comparable to measurements from single channels. The single channel I-V relationship was curvilinear and the maximum slope conductance in 40 mM Cao was 7 pS. The amplitude of unitary currents was unchanged at long times when inactivation had occurred; hence depletion is not involved in this process. Channel density was approximately 3 microns-2 and was the same for Ba and Ca currents. The whole cell asymmetry currents gave very large values for the gating charge per channel. Changes in temperature from 29 to 9 degrees C had only a slight effect on the two Ca tail current tau's at potentials where turn-on of patch and whole cell currents was markedly slowed and the peak amplitudes were reduced by one-third. Single channel recordings were obtained at these two temperatures, and the mean open time and the fast component of the closed times were scarcely affected. Unit amplitudes were reduced by 30% and the slow closed time component was doubled. Therefore, peak currents and the slow closed time component was doubled. Therefore, peak currents were reduced partly as a result of the reduction in unit amplitude, but mainly as a result of a reduction in opening probability, the latter arising from an increase of the long closed times. It is concluded that the behavior of single Ca channels in membrane patches is the same as it is in whole cells. Cooling from 29 to 9 degrees C acts primarily on transitions among closed states and has little effect on the open to closed transition.     

Cardiac Na currents and the inactivating, reopening, and waiting properties of single cardiac Na channels

Tetrodotoxin (TTX)-sensitive Na currents were examined in single dissociated ventricular myocytes from neonatal rats. Single channel and whole cell currents were measured using the patch-clamp method. The channel density was calculated as 2/micron 2, which agreed with our usual finding of four channels per membrane patch. At 20 degrees C, the single channel conductance was 20 pS. The open time distributions were fit by a single-exponential function with a mean open time of approximately 1.0 ms at membrane potentials from -60 to -40 mV. Averaged single channel and whole cell currents were similar when scaled and showed both fast and slow rates of inactivation. The inactivation and activation gating shifted quickly to hyperpolarized potentials for channels in cell-attached as well as excised patches, whereas a much slower shift occurred in whole cells. Slowly inactivating currents were present in both whole cell and single channel current measurements at potentials as positive as -40 mV. In whole cell measurements, the potential range could be extended, and slow inactivation was present at potentials as positive as -10 mV. The curves relating steady state activation and inactivation to membrane potential had very little overlap, and slow inactivation occurred at potentials that were positive to the overlap. Slow inactivation is in this way distinguishable from the overlap or window current, and the slowly inactivating current may contribute to the plateau of the rat cardiac action potential. On rare occasions, a second set of Na channels having a smaller unit conductance and briefer duration was observed. However, a separate set of threshold channels, as described by Gilly and Armstrong (1984. Nature [Lond.]. 309:448), was not found. For the commonly observed Na channels, the number of openings in some samples far exceeded the number of channels per patch and the latencies to first opening or waiting times were not sufficiently dispersed to account for the slowly inactivating currents: the slow inactivation was produced by channel reopening. A general model was developed to predict the number of openings in each sample. Models in which the number of openings per sample was due to a dispersion of waiting times combined with a rapid transition from an open to an absorbing inactivated state were unsatisfactory and a model that was more consistent with the results was identified.     

A sodium channel gating model based on single channel, macroscopic ionic, and gating currents in the squid giant axon.

Sodium channel gating behavior was modeled with Markovian models fitted to currents from the cut-open squid giant axon in the absence of divalent cations. Optimum models were selected with maximum likelihood criteria using single-channel data, then models were refined and extended by simultaneous fitting of macroscopic ionic currents, ON and OFF gating currents, and single-channel first latency densities over a wide voltage range. Best models have five closed states before channel opening, with inactivation from at least one closed state as well as the open state. Forward activation rate constants increase with depolarization, and deactivation rate constants increase with hyperpolarization. Rates of inactivation from the open or closed states are generally slower than activation or deactivation rates and show little or no voltage dependence. Channels tend to reopen several times before inactivating. Macroscopic rates of activation and inactivation result from a combination of closed, open and inactivated state transitions. At negative potentials the time to first opening dominates the macroscopic current due to slow activation rates compared with deactivation rates: channels tend to reopen rarely, and often inactivate from closed states before they reopen. At more positive potentials, the time to first opening and burst duration together produce the macroscopic current.     

Rate of opening of a population of Na channels in frog skeletal muscle fibers

Linear Systems convolution analysis of muscle sodium currents was used to predict the opening rate of sodium channels as a function of time during voltage clamp pulses. If open sodium channel lifetimes are exponentially distributed, the channel opening rate corresponding to a sodium current obtained at any particular voltage, can be analytically obtained using a simple equation, given single channel information about the mean open-channel lifetime and current.Predictions of channel opening rate during voltage clamp pulses show that sodium channel inactivation arises coincident with a decline in channel opening rate.Sodium currents pharmacologically modified with Chloramine-T treatment so that they do not inactivate, show a predicted sustained channel opening rate.Large depolarizing voltage clamp pulses produce channel opening rate functions that resemble gating currents.The predicted channel opening rate functions are best described by kinetic models for Na channels which confer most of the charge movement to transitions between closed states.Comparisons of channel opening rate functions with gating currents suggests that there may be subtypes of Na channel with some contributing more charge movement per channel opening than others.Na channels open on average, only once during the transient period of Na activation and inactivation.After transiently opening during the activation period and then closing by entering the inactivated state, Na channels reopen if the voltage pulse is long enough and contribute to steady-state currents.The convolution model overestimates the opening rate of channels contributing to the steady-state currents that remain after the transient early Na current has subsided.     

Effect of N-bromoacetamide on single sodium channel currents in excised membrane patches

We have studied the effect of N-bromoacetamide (NBA) on the behavior of single sodium channel currents in excised patches of rat myotube membrane at 10 degree C. Inward sodium currents were activated by voltage steps from holding potentials of about -100 mV to test potentials of -40 mV. The cytoplasmic-face solution was isotonic CsF. Application of NBA or pronase to the cytoplasmic face of the membrane irreversibly removed sodium channel inactivation, as determined by averaged single-channel records. Teh lifetime of the open channel at - 40 mV was increased about 10-fold by NBA treatment without affecting the amplitude of single-channel currents. A binomial analysis was used both before and after treatment to determine the number of channels within the excised patch. NBA was shown to have little effect on activation kinetics, as determined by an examination of both the rising phase of averaged currents and measurements f the delay between the start of the pulse and the first channel opening. Our data support a kinetic model of sodium channel activation in which the rate constant leading back from the open state to the last closed state is slower than expected from a strict Hodgkin-Huxley model. The data also suggest that the normal open-channel lifetime is primarily determined by the inactivation process in the voltage range we have examined.     

Shaker potassium channel gating. III: Evaluation of kinetic models for activation

Predictions of different classes of gating models involving identical conformational changes in each of four subunits were compared to the gating behavior of Shaker potassium channels without N-type inactivation. Each model was tested to see if it could simulate the voltage dependence of the steady state open probability, and the kinetics of the single-channel currents, macroscopic ionic currents and macroscopic gating currents using a single set of parameters. Activation schemes based upon four identical single-step activation processes were found to be incompatible with the experimental results, as were those involving a concerted, opening transition. A model where the opening of the channel requires two conformational changes in each of the four subunits can adequately account for the steady state and kinetic behavior of the channel. In this model, the gating in each subunit is independent except for a stabilization of the open state when all four subunits are activated, and an unstable closed conformation that the channel enters after opening. A small amount of negative cooperativity between the subunits must be added to account quantitatively for the dependence of the activation time course on holding voltage.     

Measurement of calcium channel inactivation is dependent upon the test pulse potential.

We have developed two methods to measure Ca2+ channel inactivation in Lymnaea neurons-one method, based upon the conventional double-pulse protocol, uses currents during a moderately large depolarizing pulse, and the other uses tail currents after a very strong activating pulse. Both methods avoid contamination by proton currents and are unaffected by rundown of Ca2+ current. The magnitude of inactivation measured differs for the two methods; this difference arises because the measurement of inactivation is inherently dependent upon the test pulse voltage used to monitor the Ca2+ channel conductance. We discuss two models that can generate such test pulse dependence of inactivation measurements-a two-channel model and a two-open-state model. The first model accounts for this by assuming the existence of two types of Ca2+ channels, different proportions of which are activated by the different test pulses. The second model assumes only one Ca2+ channel type, with two closed and open states; in this model, the test pulse dependence is due to the differential activation of channels in the two closed states by the test pulses. Test pulse dependence of inactivation measurements of Ca2+ channels may be a general phenomenon that has been overlooked in previous studies.     

The calcium-independent transient outward potassium current in isolated ferret right ventricular myocytes. I. Basic characterization and kinetic analysis

Enzymatically isolated myocytes from ferret right ventricles (12-16 wk, male) were studied using the whole cell patch clamp technique. The macroscopic properties of a transient outward K+ current I(to) were quantified. I(to) is selective for K+, with a PNa/PK of 0.082. Activation of I(to) is a voltage-dependent process, with both activation and inactivation being independent of Na+ or Ca2+ influx. Steady-state inactivation is well described by a single Boltzmann relationship (V1/2 = -13.5 mV; k = 5.6 mV). Substantial inactivation can occur during a subthreshold depolarization without any measurable macroscopic current. Both development of and recovery from inactivation are well described by single exponential processes. Ensemble averages of single I(to) channel currents recorded in cell-attached patches reproduce macroscopic I(to) and indicate that inactivation is complete at depolarized potentials. The overall inactivation/recovery time constant curve has a bell-shaped potential dependence that peaks between -10 and -20 mV, with time constants (22 degrees C) ranging from 23 ms (-90 mV) to 304 ms (-10 mV). Steady-state activation displays a sigmoidal dependence on membrane potential, with a net aggregate half- activation potential of +22.5 mV. Activation kinetics (0 to +70 mV, 22 degrees C) are rapid, with I(to) peaking in approximately 5-15 ms at +50 mV. Experiments conducted at reduced temperatures (12 degrees C) demonstrate that activation occurs with a time delay. A nonlinear least- squares analysis indicates that three closed kinetic states are necessary and sufficient to model activation. Derived time constants of activation (22 degrees C) ranged from 10 ms (+10 mV) to 2 ms (+70 mV). Within the framework of Hodgkin-Huxley formalism, Ito gating can be described using an a3i formulation.     

Modulation of the gating of unitary cardiac L-type Ca(2+) channels by conditioning voltage and divalent ions

Although a considerable number of studies have characterized inactivation and facilitation of macroscopic L-type Ca(2+) channel currents, the single channel properties underlying these important regulatory processes have only rarely been examined using Ca(2+) ions. We have compared unitary L-type Ca(2+) channel currents recorded with a low concentration of Ca(2+) ions with those recorded with Ba(2+) ions to elucidate the ionic dependence of the mechanisms responsible for the prepulse-dependent modulation of Ca(2+) channel gating kinetics. Conditioning prepulses were applied across a wide range of voltages to examine their effects on the subsequent Ca(2+) channel activity, recorded at a constant test potential. All recordings were made in the absence of any Ca(2+) channel agonists. Moderate-depolarizing prepulses resulted in a decrease in the probability of opening of the Ca(2+) channels during subsequent test voltage steps (inactivation), the extent of which was more dramatic with Ca(2+) ions than Ba(2+) ions. Facilitation, or increase of the average probability of opening with strong predepolarization, was due to long-duration mode 2 openings with Ca(2+) ions and Ba(2+) ions, despite a decrease in Ca(2+) channel availability (inactivation) under these conditions. The degree of both prepulse-induced inactivation and facilitation decreased with increasing Ba(2+) ion concentration. The time constants (and their proportions) describing the distributions of Ca(2+) channel open times (which reflect mode switching) were also prepulse-, and ion-dependent. These results support the hypothesis that both prior depolarization and the nature and concentration of permeant ions modulate the gating properties of cardiac L-type Ca(2+) channels.     

Mechanism of gating of T-type calcium channels

We have analyzed the gating kinetics of T-type Ca channels in 3T3 fibroblasts. Our results show that channel closing, inactivation, and recovery from inactivation each include a voltage-independent step which becomes rate limiting at extreme potentials. The data require a cyclic model with a minimum of two closed, one open, and two inactivated states. Such a model can produce good fits to our data even if the transitions between closed states are the only voltage-dependent steps in the activating pathway leading from closed to inactivated states. Our analysis suggests that the channel inactivation step, as well as the direct opening and closing transitions, are not intrinsically voltage sensitive. Single-channel recordings are consistent with this scheme. As expected, each channel produces a single burst per opening and then inactivates. Comparison of the kinetics of T-type Ca current in fibroblasts and neuronal cells reveals significant differences which suggest that different subtypes of T-type Ca channels are expressed differentially in a tissue specific manner.     

Thermodynamic entropy of two conformational transitions of single Na+ channel molecules.

Single cardiac Na+ channel currents were recorded with improved resolution (bandwidth up to 20 kHz) at two temperatures, 10 and 25 degrees C. The mean open time was determined at voltages between -50 and 0 mV by evaluation of the distribution of the event-related gaps in the center of the baseline noise. Fit of the voltage-dependent reciprocal mean open times at both temperatures allowed even for a single channel molecule to separate an entropic from an enthalpic part of activation energy for both deactivation and inactivation. Both entropies are positive and the entropy of deactivation exceeds that of inactivation by more than twice.     

The role of distal S6 hydrophobic residues in the voltage-dependent gating of CaV2.3 channels

The hydrophobic locus VAVIM is conserved in the S6 transmembrane segment of domain IV (IVS6) in Ca(V)1 and Ca(V)2 families. Herein we show that glycine substitution of the VAVIM motif in Ca(V)2.3 produced whole cell currents with inactivation kinetics that were either slower (A1719G approximately V1720G), similar (V1718G), or faster (I1721G approximately M1722G) than the wild-type channel. The fast kinetics of I1721G were observed with a approximately +10 mV shift in its voltage dependence of activation (E(0.5,act)). In contrast, the slow kinetics of A1719G and V1720G were accompanied by a significant shift of approximately -20 mV in their E(0.5,act) indicating that the relative stability of the channel closed state was decreased in these mutants. Glycine scan performed with Val (349) in IS6, Ile(701) in IIS6, and Leu(1420) in IIIS6 at positions predicted to face Val(1720) in IVS6 also produced slow inactivating currents with hyperpolarizing shifts in the activation and inactivation potentials, again pointing out a decrease in the stability of the channel closed state. Mutations to other hydrophobic residues at these positions nearly restored the channel gating. Altogether these data indicate that residues at positions equivalent to 1720 exert a critical control upon the relative stability of the channel closed and open states and more specifically, that hydrophobic residues at these positions promote the channel closed state. We discuss a three-dimensional homology model of Ca(V)2.3 based upon Kv1.2 where hydrophobic residues at positions facing Val(1720) in IS6, IIS6, and IIIS6 play a critical role in stabilizing the closed state in Ca(V)2.3.     

Inactivation viewed through single sodium channels

Recordings of the sodium current in tissue-cultured GH3 cells show that the rate of inactivation in whole cell and averaged single channel records is voltage dependent: tau h varied e-fold/approximately 26 mV. The source of this voltage dependence was investigated by examining the voltage dependence of individual rate constants, estimated by maximum likelihood analysis of single channel records, in a five-state kinetic model. The rate constant for inactivating from the open state, rather than closing, increased with depolarization, as did the probability that an open channel inactivates. The rate constant for closing from the open state had the opposite voltage dependence. Both rate constants contributed to the mean open time, which was not very voltage dependent. Both open time and burst duration were less than tau h for voltages up to -20 mV. The slowest time constant of activation, tau m, was measured from whole cell records, by fitting a single exponential either to tail currents or to activating currents in trypsin-treated cells, in which the inactivation was abolished. tau m was a bell-shaped function of voltage and had a voltage dependence similar to tau h at voltages more positive than -35 mV, but was smaller than tau h. At potentials more negative than about -10 mV, individual channels may open and close several times before inactivating. Therefore, averaged single channel records, which correspond with macroscopic current elicited by a depolarization, are best described by a convolution of the first latency density with the autocorrelation function rather than with 1 - (channel open time distribution). The voltage dependence of inactivation from the open state, in addition to that of the activation process, is a significant factor in determining the voltage dependence of macroscopic inactivation. Although the rates of activation and inactivation overlapped greatly, independent and coupled inactivation could not be statistically distinguished for two models examined. Although rates of activation affect the observed rate of inactivation at intermediate voltages, extrapolation of our estimates of rate constants suggests that at very depolarized voltages the activation process is so fast that it is an insignificant factor in the time course of inactivation. Prediction of gating currents shows that an inherently voltage-dependent inactivation process need not produce a conspicuous component in the gating current.     

A three-state model for inactivation of sodium permeability

The inactivation of Na⁺ permeability in single myelinated motor nerve fibres of Rana esculenta was investigated under voltage and current clamp conditions at 20°C in Ringer's solution and under blocked K⁺ currents. Development of inactivation and its recovery was described by two potential-dependent time constants: The smaller time constant followed the usual bell-shaped function of membrane potential, whereas the larger one was monotone-increasing with more negative potentials. Several three-state models for inactivation were investigated. The experiments could best be approximated by a model with two open and one closed state for inactivation following: open ? closed ? open. Rate constants were determined for all transitions shown from the voltage clamp experiments. The action potentials computed by means of the proposed model were in good agreement with those measured, both in Ringer's solution and under blocked K⁺ current conditions.     

Single channel studies of the phosphorylation of K+ channels in the squid giant axon. I. Steady-state conditions

Phosphorylation of the delayed rectifier channel of squid potentiates the macroscopic K+ current and slows its activation kinetics. We have studied this phenomenon at the single channel level using the cut-open axon technique under steady-state conditions. In 10 mM external K+/310 mM internal K+ there are predominantly two types of channels present, a 20-pS and a 40-pS channel. In steady state at depolarized potentials, the 40-pS channel was most active, whereas the 20-pS channel tended to disappear due to a slow inactivation process. Two methods were developed to shift the population of channels toward a dephosphorylated state. One method consisted of predialyzing a whole axon with solutions containing no ATP, while recording the currents under axial-wire voltage clamp. A piece of axon was then removed and cut open, and single channel currents were recorded from the cut-open axon. A second method was based on the difference in diffusion coefficients for ATP and proteins such as the endogenous phosphatase. The axon was cut open in a solution that did not contain Ca2+ or Cl- in order to maintain the axoplasm structurally intact and permit endogenous phosphatase to act on the membrane while ATP diffused away, before removing the axoplasm and forming a membrane patch. When dephosphorylating conditions were used, the steady-state open probability of the 40-pS channel at 42 mV was very low (less than 0.0002), and the channel openings appeared as a series of infrequent, short-duration events. The channel activity was increased up to 150-fold by photoreleasing caged ATP inside the patch pipette in the presence of the catalytic subunit of protein kinase A. The sharp increase in open probability could be accounted for by a decrease of the slow component of the closed time distribution from 23 s to 170 ms with little change in the distribution of open times (1-2 ms) and no change in the single channel current amplitude. In voltage-jump experiments the contribution of the 40-pS channel to the delayed rectifier current was often small due to the large values of the latency to the first opening.     

Cav1.4 encodes a calcium channel with low open probability and unitary conductance

When transiently expressed in tsA-201 cells, Ca(v)1.4 calcium channels support only modest whole-cell currents with unusually slow voltage-dependent inactivation kinetics. To examine the basis for this unique behavior we used cell-attached patch single-channel recordings using 100 mM external barium as the charge carrier to determine the single-channel properties of Ca(v)1.4 and to compare them to those of the Ca(v)1.2. Ca(v)1.4 channel openings occurred infrequently and were of brief duration. Moreover, openings occurred throughout the duration of the test depolarization, indicating that the slow inactivation kinetics observed at the whole-cell level are caused by sustained channel activity. Ca(v)1.4 and Ca(v)1.2 channels displayed similar latencies to first opening. Because of the rare occurrence of events, the probability of opening could not be precisely determined but was estimated to be <0.015 over a voltage range of -20 to +20 mV. The single-channel conductance of Ca(v)1.4 channels was approximately 4 pS compared with approximately 20 pS for Ca(v)1.2 under the same experimental conditions. Additionally, in the absence of divalent cations, Ca(v)1.4 channels pass cesium ions with a single-channel conductance of approximately 21 pS. Although Ca(v)1.2 opening events were best described kinetically with two open time constants, Ca(v)1.4 open times were best described by a single time constant. BayK8644 slightly enhanced the single-channel conductance in addition to increasing the open time constant for Ca(v)1.4 channels by approximately 45% without, however, causing the appearance of an additional slower gating mode. Overall, our data indicate that single Ca(v)1.4 channels support only minute amounts of calcium entry, suggesting that large numbers of these channels are needed to allow for significant whole-cell current activity, and providing a mechanism to reduce noise in the visual system.     

Acetylcholine receptor: channel-opening kinetics evaluated by rapid chemical kinetic and single-channel current measurements.

A combination of rapid chemical kinetic (quench-flow) and single-channel current measurements was used to evaluate kinetic parameters governing the opening of acetylcholine-receptor channels in the electric organ (electroplax) of Electrophorus electricus. Chemical kinetic measurements made on membrane vesicles, prepared from the E. electricus electroplax, using carbamoylcholine (200 microM-20 mM) at 12 degrees C, pH 7.0, and in the absence of a transmembrane voltage, yielded values for K1 (dissociation constant for receptor activation), phi (channel closing equilibrium constant), J (specific reaction rate for ion flux), and alpha max (maximum inactivation rate constant) of 1 mM, 3.4, 4 x 10(7) M-1 s-1, and 12 s-1, respectively. The single-channel current recordings were made with cells also from the E. electricus electroplax, at the same temperature and pH as the chemical kinetic measurements, using carbamoylcholine (50 microM-2 mM), acetylcholine (500 nM), or suberyldicholine (20 nM). Single-channel current measurements indicated the presence of a single, unique open-channel state of the E. electricus receptor, in concurrence with previous, less extensive measurements. The rate constant for channel closing (kc) obtained from the mean open time of the receptor channel is 1,100 s-1 for carbamoylcholine, 1,200 s-1 for acetylcholine, and 360 s-1 for suberyldicholine at zero membrane potential; and it decreases e-fold for an 80 mV decrease in transmembrane voltage in each case. The decrease in mean open times of the receptor channel that is associated with increasing the carbamoylcholine concentration is interpreted to be due to carbamoylcholine binding to the regulatory (inhibitory) site on the receptor. An analysis of data obtained with carbamoylcholine showed that the closed times within a burst of channel activity fit a two-exponential distribution, with a concentration-independent time constant considered to be the time constant for carbamoylcholine to dissociate from the regulatory site, and a carbamoylcholine concentration-dependent, but voltage-independent, time constant interpreted to represent the rate constant for channel opening (k0). An analysis of the mean closed time data on the basis of the minimum model gives values for K1 and k0 of 0.6 mM and 440 s-1, respectively, with carbamoylcholine as the activating ligand. The values obtained for K1, phi (= kc/k0), J, and alpha from the single-channel current measurements using electroplax are in good agreement with the values obtained from the chemical kinetic measurements using receptor-rich vesicles prepared from the same cells.(ABSTRACT TRUNCATED AT 400 WORDS)     

Sodium channels in cultured chick dorsal root ganglion neurons

Isolated Na currents were studied in cultured chick sensory neurons using the patch clamp technique. On membrane depolarization, whole cell currents showed the typical transient and voltage-dependent time course as in nerve fibres. Na currents appeared at about-40 mV and reached maximum amplitude at around-10 mV. At low voltages (-30 to 0 mV), their turning-on was sigmoidal and inactivation developed exponentially. The ratio of inactivation time constants was found to be smaller than in squid axons and comparable to that of mammalian nodes of Ranvier. Peak conductance and steady-state inactivation were strongly voltage-dependent, with maximum slopes at-17 and-40 mV, respectively. The reversal potential was close to the Nernst equilibrium potential, indicating a high degree of ion-selectivity for the channel. Addition of 3M TTX, or replacement of Na by Choline in the external bath, abolished these currents. Internal pronase (1 mg/ml) and N-bromoacetamide (0.4 mM) made inactivation incomplete, with little effect on its rate of decay.Single Na channel currents were studied in outside-out membrane patches, at potentials between-50 and-20 mV. Their activation required large negative holding potentials (-90 mV). They were fully blocked by addition of TTX (3 M) to the external bath. At-40 mV their mean open time was about 2ms and the amplitude distribution could be fitted by a single Gaussian curve, indicating the presence of a homogeneous population of channels with a conductance of 11±2 pS. Probability of opening increased and latency to first opening decreased with increasing depolarization. Inactivation of the channel became faster with stronger depolarizations, as measured from the inactivation time course of sample averages. Internal pronase (0.1 mg/ml) produced effects on inactivation comparable to those on whole cell currents. Openings of the channel had a tendency to occur in bursts and showed little inactivation during pulses of 250 ms duration. The open lifetime of the channel at low potentials (-50,-40 mV) was only three times larger than in control patches, suggesting that Na channels in chick sensory neurons can close several times before entering an inactivating absorbing state.     

Acetylcholine receptor kinetics at slow fiber neuromuscular junctions

Acetylcholine receptors in slow fiber neuromuscular junctions of garter snake (sp. Thamnophis) produced synaptic responses that were more complicated than those observed from twitch fibers. Although the slow fiber miniature end plate currents decayed monoexponentially with time, both the current fluctuations spectrum and the voltage jump end plate current required two temporal components for good theoretical fits. This behavior was accurately accounted for by a generalized version of the three-state kinetic model by del Castillo and Katz. Application of the model allowed not only the rate of channel closing to be estimated, but also the rate of channel opening (from the closed state with acetylcholine bound) and the apparent rate of acetylcholine unbinding from the receptor. The results suggest that at the peak of the miniature end plate current local receptor saturation occurs.     

Two functionally distinct 4-aminopyridine-sensitive outward K+ currents in rat atrial myocytes

In the experiments here, the detailed kinetic properties of the Ca(2+)-independent, depolarization-activated outward currents (Iout) in enzymatically dispersed adult rat atrial myocytes were studied. Although there is only slight attenuation of peak Iout during brief (100 ms) voltage steps, substantial decay is evident during long (10 s) depolarizations. The analyses here reveal that current inactivation is best described by the sum of two exponential components, which we have termed IKf and IKs to denote the fast and slow components, respectively, of Iout decay. At all test potentials, IKf inactivates approximately 20-fold more rapidly than IKs. Neither the decay time constants nor the fraction of Iout remaining at the end of 10-s depolarizations varies over the potential range of 0 to +50 mV, indicating that the rates of inactivation and recovery from inactivation are voltage independent. IKf recovers from inactivation completely, independent of the recovery of IKs, and IKf recovers approximately 20 times faster than IKs. The pharmacological properties of IKf and IKs are similar: both components are sensitive to 4-aminopyridine (1-5 mM) and both are relatively resistant to externally applied tetraethylammonium (50 mM). Taken together, these findings suggest that IKf and IKs correspond to two functionally distinct K+ currents with similar voltage-dependent properties and pharmacologic sensitivities, but with markedly different rates of inactivation and recovery from inactivation. From the experimental data, several gating models were developed in which voltage-independent inactivation is coupled either to channel opening or to the activation of the individual channel subunits. Experimental testing of predictions of these models suggests that voltage-independent inactivation is coupled to activation, and that inactivation of only a single subunit is required to result in functional inactivation of the channels. This model closely approximates the properties of IKf and IKs, as well as the composite outward currents, measured in adult rat atrial myocytes.