Inactivation properties of T-type calcium current in canine cardiac Purkinje cells.

The kinetic behavior of T-type Ca2+ current (ICa-T) was studied in canine cardiac Purkinje cells using a single suction-pipette whole-cell voltage clamp method. ICa-T was studied without contamination of conventional L-type Ca2+ current (ICa-L). Ca2+, Sr2+, or Ba2+ were used as the charge carrier. During maintained depolarization ICa-T decayed rapidly, and under most conditions the decay showed a voltage-dependent single exponential time course that did not depend on the species of charge carrier. The development of inactivation did not depend on Ca2+, but the time course required more than a single exponential process. Just negative to the threshold voltage for activating ICa-T, inactivation slowly developed and there was a delay in its onset. The time course of recovery from inactivation was dependent on the protocol used to measure it. As the duration of an inactivating voltage step was increased, recovery slowed markedly and there was a delay in its onset. The time course of recovery could be fit as a biexponential. The fast and slow time constants of recovery were relatively constant, however, the relative amplitudes were dependent on the duration of the inactivating voltage step. Recovery was not dependent on Ca2+, and it was slower at a less negative voltage. These results suggest that the T-type Ca2+ channel in cardiac Purkinje cells follows a complex kinetic scheme dependent only on voltage. This behavior can be accounted for by incorporating into a Markovian model several inactivated and closed states.     

Inactivation of voltage-gated delayed potassium current in molluscan neurons. A kinetic model.

Voltage-gated delayed potassium current in molluscan neurons is characterized by a marked inactivation. Inactivation can accumulate between repetitive pulses, giving rise to current patterns in which the maximum current during a second voltage pulse is less than the current at the end of the preceding pulse (cumulative inactivation). Other features of inactivation of this current include an onset time-course that can be characterized by the sum of two exponential processes and an early minimum in the recovery-vs.-time curve. A simple four-state model is developed that can, when supplied with rate constants derived from voltage-clamp experiments, reproduce these features of inactivation. The model incorporates state-dependent inactivation rates. Upon depolarization, both open and closed channels can be inactivated, although inactivation of closed channels is much faster. Upon repolarization, recovery from inactivated states is sufficiently slow that little recovery occurs during a short interpulse interval. Cumulative inactivation comes about as a result of fast inactivation during the second pulse, further limiting the peak current from the level at the end of the previous pulse.     

K+ channel inactivation mediated by the concerted action of the cytoplasmic N- and C-terminal domains.

We have examined the molecular mechanism of rapid inactivation gating in a mouse Shal K+ channel (mKv4.1). The results showed that inactivation of these channels follows a complex time course that is well approximated by the sum of three exponential terms. Truncation of an amphipathic region at the N-terminus (residues 2-71) abolished the rapid phase of inactivation (r = 16 ms) and altered voltage-dependent gating. Surprisingly, these effects could be mimicked by deletions affecting the hydrophilic C-terminus. The sum of two exponential terms was sufficient to describe the inactivation of deletion mutants. In fact, the time constants corresponded closely to those of the intermediate and slow phases of inactivation observed with wild-type channels. Further analysis revealed that several basic amino acids at the N-terminus do not influence inactivation, but a positively charged domain at the C-terminus (amino acids 420-550) is necessary to support rapid inactivation. Thus, the amphipathic N-terminus and the hydrophilic C-terminus of mKv4.1 are essential determinants of inactivation gating and may interact with each other to maintain the N-terminal inactivation gate near the inner mouth of the channel. Furthermore, this inactivation gate may not behave like a simple open-channel blocker because channel blockade by internal tetraethylammonium was not associated with slower current decay and an elevated external K+ concentration retarded recovery from inactivation.     

Effects of benzocaine on the kinetics of normal and batrachotoxin-modified Na channels in frog node of Ranvier.

The effects of benzocaine (0.5-1 mM) on normal Na currents, and on Na current and gating charge movement (Q) of batrachotoxin (BTX)-modified Na channels were analyzed in voltage-clamped frog node of Ranvier. Without BTX treatment the decay of Na current during pulses to between -40 and 0 mV could be decomposed into two exponential components both in the absence and in the presence of benzocaine. Benzocaine did not significantly alter the inactivation time constant of either component, but reduced both their amplitudes. The amplitude of the slow inactivating component was more decreased by benzocaine than the amplitude of the fast one, leading to an apparently faster decline of the overall Na current. After removal of Na inactivation and charge movement immobilization by BTX, benzocaine decreased the amplitude of INa with no change in time course. INa, QON, and QOFF were all reduced by the same factor. The results suggest that the rate of reaction of benzocaine with its receptor is slow compared to the rates of channel activation and inactivation. The differential effects of benzocaine on the two components of Na current inactivation in normal channels can be explained assuming two types of channel with different rates of inactivation and different affinities for the drug.     

Inactivation of batrachotoxin-modified Na+ channels in GH3 cells. Characterization and pharmacological modification

Batrachotoxin (BTX)-modified Na+ currents were characterized in GH3 cells with a reversed Na+ gradient under whole-cell voltage clamp conditions. BTX shifts the threshold of Na+ channel activation by approximately 40 mV in the hyperpolarizing direction and nearly eliminates the declining phase of Na+ currents at all voltages, suggesting that Na+ channel inactivation is removed. Paradoxically, the steady-state inactivation (h infinity) of BTX-modified Na+ channels as determined by a two-pulse protocol shows that inactivation is still present and occurs maximally near -70 mV. About 45% of BTX-modified Na+ channels are inactivated at this voltage. The development of inactivation follows a sum of two exponential functions with tau d(fast) = 10 ms and tau d(slow) = 125 ms at -70 mV. Recovery from inactivation can be achieved after hyperpolarizing the membrane to voltages more negative than -120 mV. The time course of recovery is best described by a sum of two exponentials with tau r(fast) = 6.0 ms and tau r(slow) = 240 ms at -170 mV. After reaching a minimum at -70 mV, the h infinity curve of BTX-modified Na+ channels turns upward to reach a constant plateau value of approximately 0.9 at voltages above 0 mV. Evidently, the inactivated, BTX-modified Na+ channels can be forced open at more positive potentials. The reopening kinetics of the inactivated channels follows a single exponential with a time constant of 160 ms at +50 mV. Both chloramine-T (at 0.5 mM) and alpha-scorpion toxin (at 200 nM) diminish the inactivation of BTX-modified Na+ channels. In contrast, benzocaine at 1 mM drastically enhances the inactivation of BTX-modified Na+ channels. The h infinity curve reaches minimum of less than 0.1 at -70 mV, indicating that benzocaine binds preferentially with inactivated, BTX-modified Na+ channels. Together, these results imply that BTX-modified Na+ channels are governed by an inactivation process.     

Recovery of Ca currents from inactivation: The roles of Ca influx,membrane potential,and cellular metabolism

Ca currents were examined with regard to their recovery from inactivation. The experiments were done on isolated nerve cell bodies of Helix aspersa using a combined suction pipet , microelectrode method for voltage clamp, and internal perfusion. Ca currents were separated by suppressing K and Na currents. The time course of recovery was determined by applying a test pulse at intervals ranging from 1 msec to 20 sec after prepulses varying from 20 to 3000 msec in duration. Each pair of pulses was preceded by a control pulse to ensure that the Ca currents had recovered before the next test pair was applied. Ba and Ca currents were compared and the effects of intracellular perfusion with EGTA, ATP, and vanadate were examined. Ba currents recovered in two stages and this time course was well fit by a sum of two exponentials with amplitudes and time constants given by A1 and tau 1 for the fast component and A2 and tau 2 for the slow component. In Ba the time constants were unchanged when prepulse durations were prolonged from 70 to 700 msec, although the initial amplitudes A1 and A2, particularly A2, were increased. Comparable influxes of Ca during the prepulse caused much more inactivation, but interestingly the recovery occurred at the same rate. The time course of Ca current recovery was also fit by a sum of two exponentials, the time constants of which were both smaller than the time constants of Ba current recovery. However, the time constants of Ca current recovery were increased markedly when prepulse durations were prolonged. Increasing the extracellular Ca concentration had a similar effect. Increasing the Ba influx had no effect on the recovery time constants, and the Ba results are consistent with reversible inactivation gating of potential-dependent membrane Ca channels. The Ca results show that Ca influx enhances inactivation. Intracellular perfusion with EGTA resulted in less inactivation in the cast of Ca but it had no effect on Ba currents. Intracellular ATP increased the rate of recovery of Ca currents, and intracellular vanadate inhibited recovery. It is concluded that recovery of Ca channels depends upon both Ca influx and membrane potential and is modulated by agents which affect Ca metabolism.     

Low molecular weight poly(A)+ mRNA species encode factors that modulate gating of a non-Shaker A-type K+ channel

Voltage-dependent K+ channels control repolarization of action potentials and help establish firing patterns in nerve cells. To determine the nature and role of molecular components that modulate K+ channel function in vivo, we coinjected Xenopus oocytes with cRNA encoding a cloned subthreshold A-type K+ channel (mShal1, also referred to as mKv4.1) and a low molecular weight (LMW) fraction (2-4 kb) of poly(A)+ mRNA (both from rodent brain). Coinjected oocytes exhibited a significant (fourfold) increase in the surface expression of mShal1 K+ channels with no change in the open-channel conductance. Coexpression also modified the gating kinetics of mShal1 current in several respects. Macroscopic inactivation of whole oocyte currents was fitted with the sum of two exponential components. Both fast and slow time constants of inactivation were accelerated at all membrane potentials in coinjected oocytes (tau f = 47.2 ms vs 56.5 ms at 0 mV and tau s = 157 ms vs 225 ms at 0 mV), and the corresponding ratios of amplitude terms were shifted toward domination by the fast component (Af/As = 2.71 vs 1.17 at 0 mV). Macroscopic activation was characterized in terms of the time-to-peak current, and it was found to be more rapid at all membrane potentials in coinjected oocytes (9.9 ms vs 13.5 ms at 0 mV). Coexpression also leads to more rapid recovery from inactivation (approximately 2.4-fold faster at -100 mV). The coexpressed K+ currents in oocytes resemble currents expressed in mouse fibroblasts (NIH3T3) transfected only with mShal1 cDNA. These results indicate that mammalian regulatory subunits or enzymes encoded by LMW mRNA species, which are apparently missing or expressed at low levels in Xenopus oocytes, may modulate gating in some native subthreshold A-type K+ channels.     

Properties of an early outward current in single cells of the mouse ventricle

Single ventricular myocytes of adult mice were prepared by enzymatic dissociation for voltage clamp experiments with the one suction pipette dialysis method. After blocking the Na current by 10(-4) mol/l TTX early outward currents (IEO) with incomplete inactivation could be elicited by clamping from -50 mV to test potentials (VT) positive to -30 mV. Interfering Ca currents were very small (less than 0.6 nA at VT = 0 mV). The approximation of IEO by the q4r-model showed a pronounced decrease in the time constant of activation (tau q) to more positive potentials. At 50 ms test pulses the time course of the incomplete inactivation could be described by two exponentials and a constant. The time constant of the fast exponential (tau r1) showed a slight decline towards more positive test potentials (8.1 +/- 1.0 ms at -10 mV; 5.8 +/- 1.2 ms at +50 mV, mean +/- SD, n = 5) whereas the time constant of the slow exponential (tau r2) was voltage independent (41.1 +/- 7.9 ms, mean +/- SD, n = 5). The contributions of the fast exponential and the pedestal increased towards positive test potentials. The Q10 value for the time constants of activation and fast inactivation was 2.36 +/- 0.19 and 2.51 +/- 0.09 (mean +/- SD, n = 3), respectively. After an initial delay the recovery of IEO at a recovery potential of -50 mV could be fitted monoexponentially with a time constant of 16.3 +/- 2.9 ms (mean +/- SD, n = 3). The time course of the onset of inactivation determined with the double pulse protocol was slower than the decay at the same potential, and could be described as sum of a fast (tau = 18.4 +/- 6.0 ms) and a slow (tau = 62.1 +/- 19.9ms, mean +/- SD, n = 3) exponential. IEO could be blocked completely by 1 mmol/l 4-aminopyridine at potentials up to +20 mV. Stronger depolarizations had an unblocking effect.     

Na channel activation gate modulates slow recovery from use-dependent block by local anesthetics in squid giant axons.

The time course of recovery from use-dependent block of sodium channels caused by local anesthetics was studied in squid axons. In the presence of lidocaine or its quaternary derivatives, QX-222 and QX-314, or 9-aminoacridine (9-AA), recovery from use-dependent block occurred in two phases: a fast phase and a slow phase. Only the fast phase was observed in the presence of benzocaine. The fast phase had a time constant of several milliseconds and resembled recovery from the fast Na inactivation in the absence of drug. Depending on the drug present, the magnitude of the time constant of the slow phase varied (for example at -80 mV): lidocaine, 270 ms; QX-222, 4.4 s; QX-314, 17 s; and 9-AA, 14 s. The two phases differed in the voltage dependence of recovery time constants. When the membrane was hyperpolarized, the recovery time constant for the fast phase was decreased, whereas that for the slow phase was increased for QX-compounds and 9-AA or unchanged for lidocaine. The fast phase is interpreted as representing the unblocked channels recovering from the fast Na inactivation, and the slow phase as representing the bound and blocked channels recovering from the use-dependent block accumulated by repetitive depolarizing pulse. The voltage dependence of time constants for the slow recovery is consistent with the m-gate trapping hypothesis. According to this hypothesis, the drug molecule is trapped by the activation gate (the m-gate) of the channel. The cationic form of drug molecule leaves the channel through the hydrophilic pathway, when the channel is open. However, lidocaine, after losing its proton, may leave the closed channel rapidly through the hydrophobic pathway.     

The Delay in Recovery from Fast Inactivation in Skeletal Muscle Sodium Channels Is Deactivation

1. Using macropatch techniques, we tested the assumption that deactivation underlies the observed delay in the onset to recovery from fast inactivation by comparing open-state deactivation to recovery delay for rat skeletal muscle mutations R1441C and R1441P.2. Deactivation kinetics from the open state were determined from the exponential decay of tail currents. R1441C and R1441P prolonged open-state deactivation, with the greatest effect produced by R1441P.3. Delays in the onset to recovery from fast inactivation for R1441P and for R1441C were abbreviated compared to those for rSkM1. Recovery delay was longer in R1441P than R1441C at voltages more negative than –110 mV. Recovery from inactivation exhibited a voltage dependence which, unlike delay, saturated at depolarized voltages. Recovery rate constants were increased to a similar extent for R1441C and R1441P at –150 to –120 mV compared to rSkMl.4. These results indicate that the delay in the onset to recovery from fast inactivation in skeletal muscle sodium channels is due to deactivation. Lessening of charge immobilization for R1441C and R1441P may contribute to observed biophysical defects underlying the hyperexcitability of muscle fibers containing paramyotonia congenita mutations. The second stage of recovery from fast inactivation may be affected differentially by these mutations.     

Voltage-dependent sodium channel function is regulated through membrane mechanics.

Cut-open recordings from Xenopus oocytes expressing either nerve (PN1) or skeletal muscle (SkM1) Na(+) channel alpha subunits revealed slow inactivation onset and recovery kinetics of inward current. In contrast, recordings using the macropatch configuration resulted in an immediate negative shift in the voltage-dependence of inactivation and activation, as well as time-dependent shifts in kinetics when compared to cut-open recordings. Specifically, a slow transition from predominantly slow onset and recovery to exclusively fast onset and fast recovery from inactivation occurred. The shift to fast inactivation was accelerated by patch excision and by agents that disrupted microtubule formation. Application of positive pressure to cell-attached macropatch electrodes prevented the shift in kinetics, while negative pressure led to an abrupt shift to fast inactivation. Simultaneous electrophysiological recording and video imaging of the cell-attached patch membrane revealed that the pressure-induced shift to fast inactivation coincided with rupture of sites of membrane attachment to cytoskeleton. These findings raise the possibility that the negative shift in voltage-dependence and the fast kinetics observed normally for endogenous Na(+) channels involve mechanical destabilization. Our observation that the beta1 subunit causes similar changes in function of the Na(+) channel alpha subunit suggests that beta1 may act through interaction with cytoskeleton.     

Steady-state availability of sodium channels. Interactions between activation and slow inactivation.

Changes in holding potential (Vh), affect both gating charge (the Q(Vh) curve) and peak ionic current (the F(Vh) curve) seen at positive test potentials. Careful comparison of the Q(Vh) and F(Vh) distributions indicates that these curves are similar, having two slopes (approximately 2.5e for Vh from -115 to -90 mV and approximately 4e for Vh from -90 to -65 mV) and very negative midpoints (approximately -86 mV). Thus, gating charge movement and channel availability appear closely coupled under fully-equilibrated conditions. The time course by which channels approach equilibration was explored using depolarizing prepulses of increasing duration. The high slope component seen in the F(Vh) and Q(Vh) curves is not evident following short depolarizing prepulses in which the prepulse duration approximately corresponds to the settling time for fast inactivation. Increasing the prepulse duration to 10 ms or longer reveals the high slope, and left-shifts the midpoint to more negative voltages, towards the F(Vh) and Q(Vh) distributions. These results indicate that a separate slow-moving voltage sensor affects the channels at prepulse durations greater than 10 ms. Charge movement and channel availability remain closely coupled as equilibrium is approached using depolarizing pulses of increasing durations. Both measures are 50% complete by 50 ms at a prepulse potential of -70 mV, with proportionately faster onset rates when the prepulse potential is more depolarized. By contrast, charge movement and channel availability dissociate during recovery from prolonged depolarizations. Recovery of gating charge is considerably faster than recovery of sodium ionic current after equilibration at depolarized potentials. Recovery of gating charge at -140 mV, is 65% complete within approximately 100 ms, whereas less than 30% of ionic current has recovered by this time. Thus, charge movement and channel availability appear to be uncoupled during recovery, although both rates remain voltage sensitive. These data suggest that channels remain inactivated due to a separate process operating in parallel with the fast gating charge. We demonstrate that this behavior can be simulated by a model in which the fast charge movement associated with channel activation is electrostatically-coupled to a separate slow voltage sensor responsible for the slow inactivation of channel conductance.     

Mechanism of inactivation gating of human T-type (low-voltage activated) calcium channels

Recovery from inactivation of T-type Ca channels is slow and saturates at moderate hyperpolarizing voltage steps compared with Na channels. To explore this unique kinetic pattern we measured gating and ionic currents in two closely related isoforms of T-type Ca channels. Gating current recovers from inactivation much faster than ionic current, and recovery from inactivation is much more voltage dependent for gating current than for ionic current. There is a lag in the onset of gating current recovery at -80 mV, but no lag is discernible at -120 mV. The delay in recovery from inactivation of ionic current is much more evident at all voltages. The time constant for the decay of off gating current is very similar to the time constant of deactivation of open channels (ionic tail current), and both are strongly voltage dependent over a wide voltage range. Apparently, the development of inactivation has little influence on the initial deactivation step. These results suggest that movement of gating charge occurs for inactivated states very quickly. In contrast, the transitions from inactivated to available states are orders of magnitude slower, not voltage dependent, and are rate limiting for ionic recovery. These findings support a deactivation-first path for T-type Ca channel recovery from inactivation. We have integrated these concepts into an eight-state kinetic model, which can account for the major characteristics of T-type Ca channel inactivation.     

Mutation D384N Alters Recovery of the Immobilized Gating Charge in Rat Brain IIA Sodium Channels

Rat brain (rBIIA) sodium channel fast inactivation kinetics and the time course of recovery of the immobilized gating charge were compared for wild type (WT) and the pore mutant D384N heterologously expressed in Xenopus oocytes with or without the accessory beta1-subunit. In the absence of the beta1-subunit, WT and D384N showed characteristic bimodal inactivation kinetics, but with the fast gating mode significantly more pronounced in D384N. Both, for WT and D384N, coexpression of the beta1-subunit further shifted the time course of inactivation to the fast gating mode. However, the recovery of the immobilized gating charge (Qg) of D384N was clearly faster than in WT, irrespective of the presence of the beta1-subunit. This was also reflected by the kinetics of the slow Ig OFF tail. On the other hand, the voltage dependence of the Qg-recovery was not changed by the mutation. These data suggest a direct interaction between the selectivity filter and the immobilized voltage sensor S4D4 of rBIIA sodium channels.     

Nav1.3 and FGF14 are primary determinants of the TTX-sensitive sodium current in mouse adrenal chromaffin cells

Adrenal chromaffin cells (CCs) in rodents express rapidly inactivating, tetrodotoxin (TTX)-sensitive sodium channels. The resulting current has generally been attributed to Nav1.7, although a possible role for Nav1.3 has also been suggested. Nav channels in rat CCs rapidly inactivate via two independent pathways which differ in their time course of recovery. One subpopulation recovers with time constants similar to traditional fast inactivation and the other ∼10-fold slower, but both pathways can act within a single homogenous population of channels. Here, we use Nav1.3 KO mice to probe the properties and molecular components of Nav current in CCs. We find that the absence of Nav1.3 abolishes all Nav current in about half of CCs examined, while a small, fast inactivating Nav current is still observed in the rest. To probe possible molecular components underlying slow recovery from inactivation, we used mice null for fibroblast growth factor homology factor 14 (FGF14). In these cells, the slow component of recovery from fast inactivation is completely absent in most CCs, with no change in the time constant of fast recovery. The use dependence of Nav current reduction during trains of stimuli in WT cells is completely abolished in FGF14 KO mice, directly demonstrating a role for slow recovery from inactivation in determining Nav current availability. Our results indicate that FGF14-mediated inactivation is the major determinant defining use-dependent changes in Nav availability in CCs. These results establish that Nav1.3, like other Nav isoforms, can also partner with FGF subunits, strongly regulating Nav channel function.     

Kinetic evidence for two Na channels in frog skeletal muscle

The kinetics of voltage-clamped sodium currents were studied in frog skeletal muscle. Sodium currents in frog skeletal muscle activate and inactivate following an initial delay in response to a depolarizing voltage pulse. Inactivation occurs via a double exponential decay exhibiting fast and slow components for virtually all depolarizing pulses used.The deactivation of Na currents exhibits two exponential components, one decaying rapidly, while the other decays slowly in time; the relative amplitude of the two components changes with the duration of the activating pulse. The two deactivation phases remain after pharmacological elimination of inactivation.In individual fibers, the percent amplitude of the slow inactivation component correlates with the percent amplitude of the slow deactivation component.Tetrodotoxin differentially blocks the slow deactivation component.These observations are interpreted as the activation, inactivation and deactivation of two subtypes (fast and slow) of Na channels.Studies of the slow deactivation phase magnitude vs the duration of the eliciting pulse provide a way to determine the kinetics of the slow Na channel in muscle.Ammonium substitution for Na in the Ringer produces a voltage dependent activation and inactivation of current which exhibits only one decay phase, and eliminates the slow decay phase of current, suggesting that adjustments of the ionic environment of the channels can mask the presence of one of the channel subtypes.     

Effect of ajmaline on transient outward current in rat ventricular myocytes

The mechanism of ajmaline-induced inhibition of the transient outward current (I(to)) has been investigated in right ventricular myocytes of rat using the whole cell patch clamp technique. Ajmaline decreased the amplitude and the time integral of I(to) in a concentration-dependent, but frequency- and use-independent manner. In contrast to the single exponential time course of I(to)-inactivation in control conditions (tau(i) = 37.1 +/- 2.7 ms), the apparent inactivation was fitted by a sum of two exponentials under the effect of ajmaline with concentration-dependent fast and slow components (tau(f) = 11.7 +/- 0.8 ms, tau(s) = 57.6 +/- 2.7 ms at 10 micromol/l) suggesting block development primarily in the open channel state. An improved expression enabling to calculate the association and dissociation rate constants from the concentration dependence of tau(f) and tau(s) was derived and resulted in k(on) = 4.57 x 10(6) +/- 0.32 x 10(6) mol(-1).l.s(-1) and k(off) = 20.12 +/- 5.99 s(-1). The value of K(d) = 4.4 micromol/l calculated as k(off) / k(on) was considerably lower than IC(50) = 25.9 +/- 2.9 micromol/l evaluated from the concentration dependence of the integrals of I(to). Simulations on a simple model combining Hodgkin-Huxley type gating kinetics and drug-channel interaction entirely in open channel state agreed well with the experimental data including the difference between the K(d) and IC(50). According to the model, the fraction of blocked channels increases upon depolarization and declines if depolarization is prolonged. The repolarizing step induces recovery from block with time constant of 52 ms. We conclude that in the rat right ventricular myocytes, ajmaline is an open channel blocker with fast recovery from the block at resting voltage.     

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.     

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.     

Fast inactivation of Nav current in rat adrenal chromaffin cells involves two independent inactivation pathways

Voltage-dependent sodium (Nav) current in adrenal chromaffin cells (CCs) is rapidly inactivating and tetrodotoxin (TTX)–sensitive. The fractional availability of CC Nav current has been implicated in regulation of action potential (AP) frequency and the occurrence of slow-wave burst firing. Here, through recordings of Nav current in rat CCs, primarily in adrenal medullary slices, we describe unique inactivation properties of CC Nav inactivation that help define AP firing rates in CCs. The key feature of CC Nav current is that recovery from inactivation, even following brief (5 ms) inactivation steps, exhibits two exponential components of similar amplitude. Various paired pulse protocols show that entry into the fast and slower recovery processes result from largely independent competing inactivation pathways, each of which occurs with similar onset times at depolarizing potentials. Over voltages from −120 to −80 mV, faster recovery varies from ∼3 to 30 ms, while slower recovery varies from ∼50 to 400 ms. With strong depolarization (above −10 mV), the relative entry into slow or fast recovery pathways is similar and independent of voltage. Trains of short depolarizations favor recovery from fast recovery pathways and result in cumulative increases in the slow recovery fraction. Dual-pathway fast inactivation, by promoting use-dependent accumulation in slow recovery pathways, dynamically regulates Nav availability. Consistent with this finding, repetitive AP clamp waveforms at 1–10 Hz frequencies reduce Nav availability 80–90%, depending on holding potential. These results indicate that there are two distinct pathways of fast inactivation, one leading to conventional fast recovery and the other to slower recovery, which together are well-suited to mediate use-dependent changes in Nav availability.