The pacemaker current in cardiac Purkinje myocytes

It is generally assumed that in cardiac Purkinje fibers the hyperpolarization activated inward current i(f) underlies the pacemaker potential. Because some findings are at odds with this interpretation, we used the whole cell patch clamp method to study the currents in the voltage range of diastolic depolarization in single canine Purkinje myocytes, a preparation where many confounding limitations can be avoided. In Tyrode solution ([K+]o = 5.4 mM), hyperpolarizing steps from Vh = -50 mV resulted in a time-dependent inwardly increasing current in the voltage range of diastolic depolarization. This time- dependent current (iKdd) appeared around -60 mV and reversed near EK. Small superimposed hyperpolarizing steps (5 mV) applied during the voltage clamp step showed that the slope conductance decreases during the development of this time-dependent current. Decreasing [K+]o from 5.4 to 2.7 mM shifted the reversal potential to a more negative value, near the corresponding EK. Increasing [K+]o to 10.8 mM almost abolished iKdd. Cs+ (2 mM) markedly reduced or blocked the time-dependent current at potentials positive and negative to EK. Ba2+ (4 mM) abolished the time-dependent current in its usual range of potentials and unmasked another time-dependent current (presumably i(f)) with a threshold of approximately -90 mV (> 20 mV negative to that of the time-dependent current in Tyrode solution). During more negative steps, i(f) increased in size and did not reverse. During i(f) the slope conductance measured with small (8-10 mV) superimposed clamp steps increased. High [K+]o (10.8 mM) markedly increased and Cs+ (2 mM) blocked i(f). We conclude that: (a) in the absence of Ba2+, a time-dependent current does reverse near EK and its reversal is unrelated to K+ depletion; (b) the slope conductance of that time-dependent current decreases in the absence of K+ depletion at potentials positive to EK where inactivation of iK1 is unlikely to occur. (c) Ba2+ blocks this time-dependent current and unmasks another time-dependent current (i(f)) with a more negative (> 20 mV) threshold and no reversal at more negative values; (d) Cs+ blocks both time-dependent currents recorded in the absence and presence of Ba2+. The data suggest that in the diastolic range of potentials in Purkinje myocytes there is a voltage- and time-dependent K+ current (iKdd) that can be separated from the hyperpolarization- activated inward current i(f).     

Current-dependent inactivation induced by sodium depletion in normal and batrachotoxin-treated frog node of Ranvier

In batrachotoxin (BTX)-treated frog node of Ranvier, in spite of a marked reduction in Na inactivation, the Na current still presents a time- and voltage-dependent inactivation that could induce a 50-60% decrease in the current. The inactivation was found to be modified by changing the amplitude of a conditioning pulse, adding tetrodotoxin in the external solution, or replacing NaCl with KCl in the external solution. Conditioning pulses were able to alter the reversal potential of the BTX-modified Na current (Vrev). Vrev was shifted toward negative values for inward conditioning currents and was shifted toward positive values for outward conditioning currents. The change in Vrev was proportional to the conditioning current amplitude. Large inward currents induced 15-25 mV shifts of Vrev. During a 10-20-ms depolarizing pulse, the inactivation and change in Vrev were proportional to the time integral of the current. For longer depolarizations, Vrev reached a steady state level proportional to the current amplitude. The conductance, as calculated from the current and the actual Vrev, showed an inactivation proportional to exp(Vrev F/RT). These observations suggest that the BTX-modified Na current induces a decrease in local Na concentrations, which results in an alteration of the driving force and the conductance. During a pulse that induced a large inward current, the Na space concentration [( Na]s) changed from 114 to 50-60 mM. In normal fibers, the reversal potential of Na current was also shifted toward negative values by a prepulse that induced a large inward current. The change in Vrev reached 5-15 mV, which corresponded to a decrease in [Na]s of 20-50 mM. This change in Vrev slightly altered the time course of Na current. On the basis of a three- compartment model (axoplasm-perinodal space-bulk solution), a Na permeability of the barrier between the space and the bulk solution (PNa,s) and a mean thickness of the space (theta) were calculated. The mean value of PNa,s was 0.0051 cm X s-1 in both normal and BTX-treated fibers, whereas the value of theta was 0.29 micron in BTX-treated fibers and 0.05 micron in normal fibers. When compared with the values calculated during K accumulation, PNa,s was 10 times smaller than PK,s and theta Na-BTX was equal to theta K.(ABSTRACT TRUNCATED AT 400 WORDS)     

Effect of low external calcium on the ERG current of NG108-15 cells

K(+) currents through ERG (ether-à-go-go related gene) channels were recorded in whole-cell voltage clamped NG108-15 neuroblastomaxglioma hybrid cells. The channels were fully activated by low holding potential (V(H)=-20 mV) and long depolarizing prepulses. Hyperpolarizing pulses elicited inward currents which deactivated after reaching a peak. Lowering [Ca(2+)](o) from 5 to 1. 5 or 0.5 mM decreased tau(-1), the rate constant of deactivation. The effect can be explained by a shift of the tau(-1)(V) curve to more negative potentials caused by an increase in surface charge density. Plotting tau(-1) against [Ca(2+)](o) for different potentials yielded straight lines; their slope was independent of potential at -140 to -120 mV and decreased at more positive potentials. The time to peak curve and the maximum of the steady-state inward current were also shifted to more negative potentials. In addition, peak ERG inward current increased. Raising [Ca(2+)](o) from 5 to 10 mM accelerated deactivation and decreased the peak current. 5 mM Ba(2+) affected tau(-1) similarly and inhibited peak current more strongly whereas 5 mM Mg(2+) was less potent. As found by Faravelli et al. (J. Physiol. 496 (1996) 13), bath solutions devoid of divalent cations (0 Ca(2+), 0 Mg(2+), 0.1 or 1.1 mM EGTA) abolished deactivation almost completely. The phenomenon was seen with bath containing either 40 or 6.5 mM K(+). Its occurrence was favored by raising the temperature to 34 degrees C. It suggests a particular requirement of channel closing for Ca(2+).     

Effects of membrane potential on the capacitance of skeletal muscle fibers

A method for measuring muscle fiber capacitance using small test pulses applied with the three-microelectrode voltage clamp is presented. Using this method, three membrane potential-dependent changes in capacitance were observed: (a) Capacitance of polarized fibers increased by 5--15% with depolarization from V less then -100 mV to voltages slightly below the contraction threshold. (b) Capacitance of fibers depolarized to -30 mV by 100 mM Rb solution decreased by roughly 8% with further depolarization to about +50 mV and increased with repolarization, exhibiting a maximum increase of about 10% at -80 to -90 mV. (c) Capacitance of fibers depolarized to -15 mV by 100 mM K solution increased by about 19% with further depolarization to +43 mV and decreased by about 23% with repolarization to -62 mV. Effects a and b are attributed to changes in specific membrane capacitance due to voltage-dependent redistribution of mobile charged groups within surface of T-tubule membranes. Effect c is caused by changes in the T-system space constant lambdaT due to the voltage dependence of K conductance (inward rectification). Analysis of c showed that in 100 mM K solution lambdaT congruent to 30 mum when inward rectification was fully activated by hyperpolarization and that the density of inward rectifier channels is about the same in surface and tubular membranes. Fiber internal resistance was found to be independent of voltage, a necessary condition for the interpretation of the capacitance measurements.     

Na/K pump current in aggregates of cultured chick cardiac myocytes

Spontaneously beating aggregates of cultured embryonic chick cardiac myocytes, maintained at 37 degrees C, were voltage clamped using a single microelectrode switching clamp to measure the current generated by the Na/K pump (Ip). In resting, steady-state preparations an ouabain-sensitive current of 0.46 +/- 0.03 microA/cm2 (n = 22) was identified. This current was not affected by 1 mM Ba, which was used to reduce inward rectifier current (IK1) and linearize the current-voltage relationship. When K-free solution was used to block Ip, subsequent addition of Ko reactivated the Na/K pump, generating an outward reactivation current that was also ouabain sensitive. The reactivation current magnitude was a saturating function of Ko with a Hill coefficient of 1.7 and K0.5 of 1.9 mM in the presence of 144 mM Nao. The reactivation current was increased in magnitude when Nai was increased by lengthening the period of time that the preparation was exposed to K-free solution prior to reactivation. When Nai was raised by 3 microM monensin, steady-state Ip was increased more than threefold above the resting value to 1.74 +/- 0.09 microA/cm2 (n = 11). From these measurements and other published data we calculate that in a resting myocyte: (a) the steady-state Ip should hyperpolarize the membrane by 6.5 mV, (b) the turnover rate of the Na/K pump is 29 s-1, and (c) the Na influx is 14.3 pmol/cm2.s. We conclude that in cultured embryonic chick cardiac myocytes, the Na/K pump generates a measurable current which, under certain conditions, can be isolated from other membrane currents and has properties similar to those reported for adult cardiac cells.     

Measurement of Na-K pump current in acinar cells of rat lacrimal glands.

Isolated cells from rat lacrimal glands were voltage clamped using the tight-seal whole-cell recording technique. The intracellular solution contained ATP and an elevated Na concentration (70 mM). Removing external K ions elicited an inward current shift. Ouabain (0.5 mM) induced an inward current shift of identical amplitude, but with slower kinetics. In the presence of ouabain, removal of K ions did not alter the cell current. The potassium- and ouabain-sensitive current was outward between -120 and +20 mV, and its amplitude decreased below -60 mV. This current was highly sensitive to temperature, and was not affected by blockers of the K channels which are present in these cells. It was attributed to an inhibition of the Na-K pump. The Na-K pump current was estimated to be 15 pA for an average acinar cell at physiological temperature, with 70 mM internal Na ions and 20 mM external K ions. Implications of this value in terms of electrolyte secretion are discussed.     

The comparison of the estimation of enzyme kinetic parameters by fitting reaction curve to the integrated Michaelis-Menten rate equations of different predictor variables

The estimation of enzyme kinetic parameters by nonlinear fitting reaction curve to the integrated Michaelis-Menten rate equation ln(S(0)/S)+(S(0)-S)/K(m)=(V(m)/K(m))xt was investigated and compared to that by fitting to (S(0)-S)/t=V(m)-K(m)x[ln(S(0)/S)/t] (Atkins GL, Nimmo IA. The reliability of Michaelis-Menten constants and maximum velocities estimated by using the integrated Michaelis-Menten equation. Biochem J 1973;135:779-84) with uricase as the model. Uricase reaction curve was simulated with random absorbance error of 0.001 at 0.075 mmol/l uric acid. Experimental reaction curve was monitored by absorbance at 293 nm. For both CV and deviation <20% by simulation, K(m) from 5 to 100 micromol/l was estimated with Eq. (1) while K(m) from 5 to 50 micromol/l was estimated with Eq. (2). The background absorbance and the error in the lag time of steady-state reaction resulted in negative K(m) with Eq. (2), but did not affect K(m) estimated with Eq. (1). Both equations gave better estimation of V(m). The computation time and the goodness of fit with Eq. (1) were 40-fold greater than those with Eq. (2). By experimentation, Eq. (1) yielded K(m) consistent with the Lineweaver-Burk plot analysis, but Eq. (2) gave many negative parameters. Apparent K(m) by Eq. (1) linearly increased, while V(m) were constant, vs. xanthine concentrations, and the inhibition constant was consistent with the Lineweaver-Burk plot analysis. These results suggested that the integrated rate equation that uses the predictor variable of reaction time was reliable for the estimation of enzyme kinetic parameters and applicable for the characterization of enzyme inhibitors.     

Effects of external Rb+ on inward rectifier K+ channels of bovine pulmonary artery endothelial cells

Inward rectifier (IR) K+ channels of bovine pulmonary artery endothelial cells were studied using the whole-cell, cell-attached, and outside-out patch-clamp configurations. The effects of Rb+ on the voltage dependence and kinetics of IR gating were explored, with [Rb+]o + [K+]o = 160 mM. Partial substitution of Rb+ for K+ resulted in voltage-dependent reduction of inward currents, consistent with Rb+ being a weakly permeant blocker of the IR. In cells studied with a K(+)- free pipette solution, external Rb+ reduced inward IR currents to a similar extent at large negative potentials but block at more positive potentials was enhanced. In outside-out patches, the single-channel i-V relationship was approximately linear in symmetrical K+, but rectified strongly outwardly in high [Rb+]o due to a reduced conductance for inward current. The permeability of Rb+ based on reversal potential, Vrev, was 0.45 that of K+, whereas the Rb+ conductance was much lower, 0.034 that of K+, measured at Vrev-80 mV. The steady state voltage- dependence of IR gating was determined in Rb(+)-containing solutions by applying variable prepulses, followed by a test pulse to a potential at which outward current deactivation was observed. As [Rb+]o was increased, the half-activation potential, V1/2, changed less than Vrev. In high [K+]o solutions V1/2 was Vrev-6 mV, while in high [Rb+]o V1/2 was Vrev + 7 mV. This behavior contrasts with the classical parallel shift of V1/2 with Vrev in K+ solutions. Steady state IR gating was less steeply voltage-dependent in high [Rb+]o than in K+ solutions, with Boltzmann slope factors of 6.4 and 4.4 mV, respectively. Rb+ decreased (slowed) both activation and deactivation rate constants defined at V1/2, and decreased the steepness of the voltage dependence of the activation rate constant by 42%. Deactivation of IR channels in outside-out patches was also slowed by Rb+. In summary, Rb+ can replace K+ in setting the voltage-dependence of IR gating, but in doing so alters the kinetics.     

Calcium channel currents in isolated smooth muscle cells from human bronchus

An electrophysiological study was carried out on smooth muscle cells that were enzymatically dissociated from bundles of muscle fibers dissected out of human bronchi obtained at thoracotomy. These cells that retain the contractile properties of intact bundles were voltage-clamped by means of the whole-cell patch-clamp technique. Upon voltage steps from a holding potential of -60 mV to more positive levels, the initial inward current was followed by large outward currents that inactivated slowly. These were subsequently reduced by substituting Cs+ for K+ in the internal solution and by using Ba2+ instead of Ca2+ as a charge carrier in the external solution. Under these conditions, the inward current did not completely inactivate in the course of 300-ms voltage steps. Inward current measured after leak subtraction was activated at a membrane potential of -25.8 +/- 5 mV, was maximum at +18 +/- 4 mV, and had an apparent reversal potential of +52.5 +/- 5.5 mV (n = 5). The potential at which steady-state inactivation was half-maximum was -28 mV (n = 5). This inward current was identified as a calcium current on the following basis: 1) it was not altered by 10 microM tetrodotoxin (TTX) or by lowering to 10 mM external Na+ concentration; 2) it was blocked by 2.5 mM Co2+ or 1 microM PN 200-110; 3) it was enhanced by 1 microM BAY K 8644, which in addition suppressed the PN 200-110 blockade.(ABSTRACT TRUNCATED AT 250 WORDS)     

Probing the geometry of the inner vestibule of BK channels with sugars

The geometry of the inner vestibule of BK channels was probed by examining the effects of different sugars in the intracellular solution on single-channel current amplitude (unitary current). Glycerol, glucose, and sucrose decreased unitary current through BK channels in a concentration- and size-dependent manner, in the order sucrose > glucose > glycerol, with outward currents being reduced more than inward currents. The fractional decrease of outward current was more directly related to the fractional hydrodynamic volume occupied by the sugars than to changes in osmolality. For concentrations of sugars < or =1 M, the i/V plots for outward currents in the presence and absence of sugar superimposed after scaling, and increasing K(+)(i) from 150 mM to 2 M increased the magnitudes of the i/V plots with little effect on the shape of the scaled curves. These observations suggest that sugars < or =1 M reduce outward currents mainly by entering the inner vestibule and reducing the movement of K(+) through the vestibule, rather than by limiting diffusion-controlled access of K(+) to the vestibule. With 2 M sucrose, the movement of K(+) into the inner vestibule became diffusion limited for 150 mM K(+)(i) and voltages > +100 mV. Increasing K(+)(i) then relieved the diffusion limitation. An estimate of the capture radius based on the 5 pA diffusion-limited current for channels without the ring of negative charge at the entrance to the inner vestibule was 2.2 A. Adding the radius of a hydrated K(+) (6-8 A) then gave an effective radius for the entrance to the inner vestibule of 8-10 A. Such a functionally wide entrance to the inner vestibule together with our observation that even small concentrations of sugar in the inner vestibule reduce unitary current suggest that a wide inner vestibule is required for the large conductance of BK channels.     

Activation of ATP-dependent K+ currents in intact skeletal muscle fibres by reduced intracellular pH.

We have used three-microelectrode voltage clamp in conjunction with the ammonium prepulse method to investigate the effects of lowered intracellular pH (pHi) on resting potassium currents of frog skeletal muscle fibres. Potassium currents were recorded in 40 mM K+, Cl(-)-free solution in response either to voltage steps or ramps. An ammonium prepulse (2 h) reduced pHi to 6.45 from a control value of 7.19. The intracellular ATP concentration, measured with high-pressure liquid chromatography (HPLC), was unchanged by this procedure. Mean outward potassium currents were larger in low pHi than in control fibres, being about twice as large at +40 mV, whereas mean inward currents were very similar in control and low-pHi fibres. The sulphonylurea glibenclamide blocked single KATP channels in excised patches with a Kd of 3 microM. In intact fibres 50 microM glibenclamide had no effect on K+ currents in controls but reduced currents in low-pHi fibres. In the presence of glibenclamide, K+ currents in low-pHi fibres were not significantly different from those in control fibres. We suggest that reduced pHi in intact skeletal muscle fibres opens ATP-dependent potassium channels (KATP channels), as has been shown to occur in excised patches of membrane.     

Control of ion distribution in isolated smooth muscle cells. I. Potassium

We describe a technique for examining unidirectional ion movements in suspensions of enzymatically disaggregated smooth muscle cells derived from stomach muscle of the toad. This technique has been used to analyze the movement of 42K across these cells. This analysis was greatly simplified by the finding that the cells were in a steady state with respect to K+ distribution after isolation. The potassium contents of the isolated cells were identical to those of intact smooth muscle (131 mM/liter intracellular fluid) and stable for over 4 h; moreover, the unidirectional influx and efflux rates were equal. An additional simplification was provided by the finding that virtually all the K+ exchanges in a manner predicted for a simple two-compartment system consisting of an extracellular and an intracellular space. Transmembrane K+ flux in these cells averaged 1.2 pmol.cm-2.s-1 at room temperature. A large portion (approximately 80%) of 42K influx appeared to be mediated by a saturable transport system with an apparent Km of 0.6 mM and an apparent Vmax of 1.3 pmol.cm-2.s-1. The calculated resting membrane permeability to K+ in these isolated smooth muscle cells, assuming a membrane potential of -50 mV, was 2.9 X 10(-8) cm/s. The calculated gK+ was 2.7 mumho/cm2 constituting only a small fraction of the total membrane conductance as measured electrophysiologically. The latter finding suggests that the resting membrane potential in the isolated cells must be determined by ions in addition to K+. We propose that these methods for studying ion movements in smooth muscle should aid in unraveling the mechanisms responsible for controlling the distribution of ions both at rest, as in the present study, as well as in response to neurotransmitters.     

Single-channel, macroscopic, and gating currents from sodium channels in the squid giant axon.

Single-channel, macroscopic ionic, and macroscopic gating currents were recorded from the voltage-dependent sodium channel using patch-clamp techniques on the cut-open squid giant axon. To obtain a complete set of physiological measurements of sodium channel gating under identical conditions, and to facilitate comparison with previous work, comparison was made between currents recorded in the absence of extracellular divalent cations and in the presence of physiological concentrations of extracellular Ca2+ (10 mM) and Mg2+ (50 mM). The single-channel currents were well resolved when divalent cations were not included in the extracellular solution, but were decreased in amplitude in the presence of Ca2+ and Mg2+ ions. The instantaneous current-voltage relationship obtained from macroscopic tail current measurements similarly was depressed by divalents, and showed a negative slope-conductance region for inward current at negative potentials. Voltage dependent parameters of channel gating were shifted 9-13 mV towards depolarized potentials by external divalent cations, including the peak fraction of channels open versus voltage, the time constant of tail current decline, the prepulse inactivation versus voltage relationship, and the charge-voltage relationship for gating currents. The effects of divalent cations are consistent with open channel block by Ca2+ and Mg2+ together with divalent screening of membrane charges.     

Asymmetry currents and admittance in squid axons.

The complex admittance of squid (Loligo pealei) axon was measured rapidly (within 1 s) with pseudo-random small signals and discrete Fourier transform techniques under guarded, "space-clamp" conditions and during suppression of ion conduction. Asymmetry currents were measured by paired step clam pulses of +/-70 mV from a holding potential of -97 mV and gave an apparent capacitance of 0.36 muF/cm2. However, the admittance data showed no change in capacitance at holding potentials from -97 to -67 mV and gave a decrease of 0.07 of 0.15 muF/cm2 at -37 mV. The failure to observe a capacitance increase at low membrane potentials suggests the following possibilities: (a) the asymmetry current is a displacement current that inactivates completely with time, and (b) the asymmetry current is not a displacement current and arises from large signal effects (i.e., delayed nonlinearity in ionic current) on the membrane.     

Intramembranous charge movement in frog cut twitch fibers mounted in a double vaseline-gap chamber

Intramembranous charge movement was measured in cut twitch fibers mounted in a double Vaseline-gap chamber with either a tetraethylammonium chloride (TEA.Cl) or a TEA2.SO4 solution (13-14 degrees C) in the central pool. Charge vs. voltage data were fitted by a single two-state Boltzmann distribution function. The average values of V (the voltage at which steady-state charge is equally distributed between the two Boltzmann states), k (the voltage dependence factor), and qmax/cm (the maximum charge divided by the linear capacitance, both per unit length of fiber) were V = -53.3 mV (SEM, 1.1 mV), k = 6.3 mV (SEM, 0.3 mV), qmax/cm = 18.0 nC/microF (SEM, 1.1 nC/microF) in the TEA.Cl solution; and V = -35.1 mV (SEM, 1.8 mV), k = 10.5 mV (SEM, 0.9 mV), qmax/cm = 36.3 nC/microF (SEM, 3.2 nC/microF) in the TEA2.SO4 solution. These values of k are smaller than those previously reported for cut twitch fibers and are as small as those reported for intact fibers. If a correction is made for the contributions of currents from under the Vaseline seals, V = -51.2 mV (SEM, 1.1 mV), k = 7.2 mV (SEM, 0.4 mV), qmax/cm = 22.9 nC/microF (SEM, 1.4 nC/microF) in the TEA.Cl solution; and V = -34.0 mV (SEM, 1.9 mV), k = 10.1 mV (SEM, 1.1 mV), qmax/cm = 38.8 nC/microF (SEM, 3.2 nC/microF) in the TEA2.SO4 solution. With this correction, however, the fit of the theoretical curve to the data is poor. A good fit with this correction can be obtained with a sum of two Boltzmann distribution functions. The first has average values V = -33.0 mV (SEM, 2.8 mV), k = 11.0 mV (SEM, 0.5 mV), qmax/cm = 10.6 nC/microF (SEM, 1.0 nC/microF) in the TEA.Cl solution; and V = -20.0 mV (SEM, 3.3 mV), k = 17.0 mV (SEM, 2.0 mV), qmax/cm = 36.4 nC/microF (SEM, 2.3 nC/microF) in the TEA2.SO4 solution. The second has average values V = -56.5 mV (SEM, 1.3 mV), k = 2.9 mV (SEM, 0.4 mV), qmax/cm = 13.2 nC/microF (SEM, 1.0 nC/microF) in the TEA.Cl solution; and V = -41.6 mV (SEM, 1.4 mV), k = 2.5 mV (SEM, 0.8 mV), qmax/cm = 11.8 nC/microF (SEM, 1.7 nC/microF) in the TEA2.SO4 solution. When a fiber is depolarized to near V of the second Boltzmann function, a slowly developing "hump" appears in the ON-segment of the current record.(ABSTRACT TRUNCATED AT 400 WORDS)     

Voltage-dependent and odorant-regulated currents in isolated olfactory receptor neurons of the channel catfish.

The electrical properties of olfactory receptor neurons, enzymatically dissociated from the channel catfish (Ictalurus punctatus), were studied using the whole-cell patch-clamp technique. Six voltage-dependent ionic currents were isolated. Transient inward currents (0.1-1.7 nA) were observed in response to depolarizing voltage steps from a holding potential of -80 mV in all neurons examined. They activated between -70 and -50 mV and were blocked by addition of 1 microM tetrodotoxin (TTX) to the bath or by replacing Na+ in the bath with N-methyl-D-glucamine and were classified as Na+ currents. Sustained inward currents, observed in most neurons examined when Na+ inward currents were blocked with TTX and outward currents were blocked by replacing K+ in the pipette solution with Cs+ and by addition of 10 mM Ba2+ to the bath, activated between -40 and -30 mV, reached a peak at 0 mV, and were blocked by 5 microM nimodipine. These currents were classified as L-type Ca2+ currents. Large, slowly activating outward currents that were blocked by simultaneous replacement of K+ in the pipette with Cs+ and addition of Ba2+ to the bath were observed in all olfactory neurons examined. The outward K+ currents activated over approximately the same range as the Na+ currents (-60 to -50 mV), but the Na+ currents were larger at the normal resting potential of the neurons (-45 +/- 11 mV, mean +/- SD, n = 52). Four different types of K+ currents could be differentiated: a Ca(2+)-activated K+ current, a transient K+ current, a delayed rectifier K+ current, and an inward rectifier K+ current. Spontaneous action potentials of varying amplitude were sometimes observed in the cell-attached recording configuration. Action potentials were not observed in whole-cell recordings with normal internal solution (K+ = 100 mM) in the pipette, but frequently appeared when K+ was reduced to 85 mM. These observations suggest that the membrane potential and action potential amplitude of catfish olfactory neurons are significantly affected by the activity of single channels due to the high input resistance (6.6 +/- 5.2 G omega, n = 20) and low membrane capacitance (2.1 +/- 1.1 pF, n = 46) of the cells.(ABSTRACT TRUNCATED AT 400 WORDS)     

Inward rectifier K+-channel kinetics from analysis of the complex conductance of Aplysia neuronal membrane.

Conduction in inward rectifier, K+-channels in Aplysia neuron and Ba++ blockade of these channels were studied by rapid measurement of the membrane complex admittance in the frequency range 0.05 to 200 Hz during voltage clamps to membrane potentials in the range -90 to -40 mV. Complex ionic conductances of K+ and Cl- rectifiers were extracted from complex admittances of other membrane conduction processes and capacitance by vector subtraction of the membrane complex admittance during suppressed inward K+ current (near zero-mean current and in zero [K+]0) from complex admittances determined at other [K+]0 and membrane potentials. The contribution of the K+ rectifier to the admittance is distinguishable in the frequency domain above 1 Hz from the contribution of the Cl- rectifier, which is only apparent at frequencies less than 0.1 Hz. The voltage dependence (-90 to -40 mV) of the chord conductance (0.2 to 0.05 microS) and the relaxation time (4-8 ms) of K+ rectifier channels at [K+]0 = 40 mM were determined by curve fits of admittance data by a membrane admittance model based on the linearized Hodgkin-Huxley equations. The conductance of inward rectifier, K+ channels at a membrane potential of -80 mV had a square-root dependence on external K+ concentration, and the relaxation time increased from 2 to 7.5 ms for [K+]0 = 20 and 100 mM, respectively. The complex conductance of the inward K+ rectifier, affected by Ba++, was obtained by complex vector subtraction of the membrane admittance during blockage of inward rectifier, K+ channels (at -35 mV and [Ba++]0 = 5 mM) from admittances determined at -80 mV and at other Ba++ concentrations. The relaxation time of the blockade process decreased with increases in Ba++ concentration. An open-closed channel state model produces the inductive-like kinetic behavior in the complex conductance of inward rectifier, K+ channels and the addition of a blocked channel state accounts for the capacitive-like kinetic behavior of the Ba++ blockade process.     

Voltage-dependent calcium and calcium-activated potassium currents of a molluscan photoreceptor

Two-microelectrode voltage clamp studies were performed on the somata of Hermissenda Type B photoreceptors that had been isolated by axotomy from all synaptic interaction as well as any impulse-generating (i.e., active) membrane. In the presence of 2-10 mM 4-aminopyridine (4-AP) and 100 mM tetraethylammonium ion (TEA), which eliminated two previously described voltage-dependent potassium currents (IA and the delayed rectifier), a voltage-dependent outward current was apparent in the steady state responses to command voltage steps more positive than -40 mV (absolute). This current increased with increasing external Ca++. The magnitude of the outward current decreased and an inward current became apparent following EGTA injection. Substitution of external Ba++ for Ca++ also made the inward current more apparent. This inward current, which was almost eliminated after being exposed for approximately 5 min to a solution in which external Ca++ was replaced with Cd++, was maximally activated at approximately 0 mV. Elevation of external potassium allowed the calcium (ICa++) and calcium-dependent K+ (IC) currents to be substantially separated. Command pulses to 0 mV elicited maximal ICa++ but no IC because no K+ currents flowed at their new reversal potential (0 mV) in 300 mM K+. At a holding potential of -60 mV, which was now more negative than the potassium equilibrium potential, EK+, in 300 mM K+, IC appeared as an inward tail current after positive command steps. The voltage dependence of ICa++ was demonstrated with positive steps in 100 mM Ba++, 4-AP, and TEA. Other data indicated that in 10 mM Ca++, IC underwent pronounced and prolonged inactivation whereas ICa++ did not. When the photoreceptor was stimulated with a light step (with the membrane potential held at -60 mV), there was also a prolonged inactivation of IC. In elevated external Ca++, ICa++ also showed similar inactivation. These data suggest that IC may undergo prolonged inactivation due to a direct effect of elevated intracellular Ca++, as was previously shown for a voltage-dependent potassium current, IA. These results are discussed in relation to the production of training-induced changes of membrane currents on retention days of associative learning.     

K+ channels of stomatal guard cells. Characteristics of the inward rectifier and its control by pH

Intracellular microelectrode recordings and a two-electrode voltage clamp have been used to characterize the current carried by inward rectifying K+ channels of stomatal guard cells from the broadbean, Vicia faba L. Superficially, the current displayed many features common to inward rectifiers of neuromuscular and egg cell membranes. In millimolar external K+ concentrations (Ko+), it activated on hyperpolarization with half-times of 100-200 ms, showed no evidence of time- or voltage-dependent inactivation, and deactivated rapidly (tau approximately 10 ms) on clamping to 0 mV. Steady-state conductance-voltage characteristics indicated an apparent gating charge of 1.3-1.6. Current reversal showed a Nernstian dependence on Ko+ over the range 3-30 mM, and the inward rectifier was found to be highly selective for K+ over other monovalent cations (K+ greater than Rb+ greater than Cs+ much greater than Na+). Unlike the inward rectifiers of animal membranes, the current was blocked by charybdotoxin and alpha-dendrotoxin (Kd much less than 50 nM), as well as by tetraethylammonium chloride (K1/2 = 9.1 mM); gating of the guard cell K+ current was fixed to voltages near -120 mV, independent of Ko+, and the current activated only with supramillimolar K+ outside (EK+ greater than -120 mV). Most striking, however, was inward rectifier sensitivity to [H+] with the K+ current activated reversibly by mild acid external pH. Current through the K+ inward rectifier was found to be largely independent of intracellular pH and the current reversal (equilibrium) potential was unaffected by pHo from 7.4 to 5.5. By contrast, current through the K+ outward rectifier previously characterized in these cells (1988. J. Membr. Biol. 102:235) was largely insensitive to pHo, but was blocked reversibly by acid-going intracellular pH. The action of pHo on the K+ inward rectifier could not be mimicked by extracellular Ca2+ for which changes in activation, deactivation, and conductance were consonant with an effect on surface charge ([Ca2+] less than or equal to 1 mM). Rather, extracellular pH affected activation and deactivation kinetics disproportionately, with acid-going pHo raising the K+ conductance and shifting the conductance-voltage profile positive-going along the voltage axis and into the physiological voltage range. Voltage and pH dependencies for gating were consistent with a single, titratable group (pKa approximately 7 at -200 mV) residing deep within the membrane electric field and accessible from the outside.(ABSTRACT TRUNCATED AT 400 WORDS)     

Coupled K+-water flux through the HERG potassium channel measured by an osmotic pulse method

The streaming potential (V(stream)) is a signature feature of ion channels in which permeating ions and water molecules move in a single file. V(stream) provides a quantitative measure of the ion and water flux (the water-ion coupling ratio), the knowledge of which is a prerequisite for elucidating the mechanisms of ion permeation. We have developed a method to measure V(stream) with the whole-cell patch-clamp configuration. A HEK293 cell stably expressing the HERG potassium channel was voltage clamped and exposed to hyperosmotic solutions for short periods of time (<1 s) by an ultrafast solution switching system (the osmotic pulse [quick jump-and-away] method). The reversal potentials were monitored by a series of voltage ramps before, during, and after the osmotic pulse. The shifts of the reversal potentials immediately after the osmotic jump gave V(stream). In symmetrical K+ solutions (10 mM), the V(stream)s measured at different osmolalities showed a linear relationship with a slope of -0.7 mV/DeltaOsm, from which the water-ion coupling ratio (n, the ratio of the flux of water to the flux of cations; Levitt, D.G., S.R. Elias, and J.M. Hautman. 1978. Biochim. Biophys. Acta. 512:436-451) was calculated to be 1.4. In symmetrical 100 mM K+ solutions, the coupling ratio was decreased significantly (n = 0.9), indicating that the permeation process through states with increased ion occupancy became significant. We presented a diagrammatic representation linking the water-ion coupling ratio to the mode of ion permeation and suggested that the coupling ratio of one may represent the least hydrated ion flux in the single-file pore.