Acute thyroid hormone promotes slow inactivation of sodium current in neonatal cardiac myocytes.

Sodium current (INa) inactivation kinetics in neonatal cardiac myocytes were analyzed using whole cell voltage clamp before and after acute treatments with thyroid hormone (3,5,3'-triiodo-L-thyronine, T3). In untreated neonatal myocytes, INa inactivation was predominantly mono-exponential, with 93 +/- 3% (S.D.; n = 9) of the peak amplitude decaying with a time constant, tau h1, of 1.8 +/- 0.5 ms at -30 mV. The remaining 7% of control INa decayed more slowly, with a time constant, tau h2, of 9.3 +/- 3.0 ms at -30 mV. The contribution of slowly-inactivating channels to peak current was increased from 7% to 43 +/- 27% within 5 min of exposure to 5-20 nM T3 (nine cells; P less than 0.005). The time constants for both the fast- and slow-inactivating components of peak current (tau h1 and tau h2) were not significantly changed by acute T3 treatment, nor was steady-state INa inactivation (h infinity) affected. Thyroid hormone action on sodium inactivation was partially reversible by lidocaine. These findings indicate that T3 acts at the neonatal cardiac cell membrane to promote slow inactivation kinetics in sodium channels.     

Inactivation of Ca2+ release channels (ryanodine receptors RyR1 and RyR2) with rapid steps in [Ca2+] and voltage.

The transient responses of sheep cardiac and rabbit skeletal ryanodine receptors (RyRs) to step changes in membrane potential and cytosolic [Ca2+] were measured. Both cardiac and skeletal RyRs have two voltage-dependent inactivation processes (tau approximately 1-3 s at +40 mV) that operate at opposite voltage extremes. Approximately one-half to two-thirds of RyRs inactivated when the bilayer voltage was stepped either way between positive and negative values. Inactivation was not detected (within 30 s) in RyRs with Po less than 0.2. Inactivation rates increased with intraburst open probability (Po) and in proportion to the probability of a long-lived, RyR open state (P(OL)) RyR inactivation depended on P(OL) and not on the particular activator (Ca2+ (microM), ATP, caffeine, and ryanodine), inhibitor (mM Ca2+ and Mg2+), or gating mode. The activity of one-half to two-thirds of RyRs declined (i.e., the RyRs inactivated) after [Ca2+] steps from subactivating (0.1 microM) to activating (1-100 microM) levels. This was due to the same inactivation mechanism responsible for inactivation after voltage steps. Both forms of inactivation had the same kinetics and similar dependencies on Po and voltage. Moreover, RyRs that failed to inactivate after voltage steps also did not inactivate after [Ca2+] steps. The inactivating response to [Ca2+] steps (0.1-1 microM) was not RyRs "adapting" to steady [Ca2+] after the step, because a subsequent step from 1 to 100 microM failed to reactivate RyRs.     

Blockade of sodium channels by Bistramide A in voltage-clamped frog skeletal muscle fibres.

The effect of Bistramide A, a toxin isolated from Bistratum lissoclinum Sluiter (Urochordata), on the peak sodium current (INa) of frog skeletal muscle fibres was studied with the double sucrose gap voltage clamp technique. External or internal application of Bistramide A inhibited INa without alteration of the kinetic parameters of the current nor of the apparent reversal potential for Na. The steady-state activation curve of INa was unchanged while the steady-state inactivation curve of INa was shifted towards more negative membrane potentials. Dose-response curves indicated an apparent dissociation constant for Bistramide A of 3.3 microM and a Hill coefficient of 1.2 which suggested a one to one relation between the toxin and Na channel. The inhibition of INa occurred at rest, and was more important at more positive holding potentials. Bistramide A exhibited only a weak frequency-dependent effect. The toxin did not interact with the use-dependent effect of lidocaine. It mainly blocked Na channels at more depolarized holding potentials. The toxin blocked Na channels when it was internally applyed and when the inactivation gating system has been previously destroyed by internal diffusion of iodate. The data suggest that Bistramide A inhibited the Na channel both at rest and in the inactivated state and occupied a site which was not located on the inactivation gate.     

Tetrodotoxin block of sodium channels in rabbit Purkinje fibers. Interactions between toxin binding and channel gating

Tetrodotoxin (TTX) block of cardiac sodium channels was studied in rabbit Purkinje fibers using a two-microelectrode voltage clamp to measure sodium current. INa decreases with TTX as if one toxin molecule blocks one channel with a dissociation constant KD approximately equal to 1 microM. KD remains unchanged when INa is partially inactivated by steady depolarization. Thus, TTX binding and channel inactivation are independent at equilibrium. Interactions between toxin binding and gating were revealed, however, by kinetic behavior that depends on rates of equilibration. For example, frequent suprathreshold pulses produce extra use-dependent block beyond the tonic block seen with widely spaced stimuli. Such lingering aftereffects of depolarization were characterized by double-pulse experiments. The extra block decays slowly enough (tau approximately equal to 5 s) to be easily separated from normal recovery from inactivation (tau less than 0.2 s at 18 degrees C). The amount of extra block increases to a saturating level with conditioning depolarizations that produce inactivation without detectable activation. Stronger depolarizations that clearly open channels give the same final level of extra block, but its development includes a fast phase whose voltage- and time-dependence resemble channel activation. Thus, TTX block and channel gating are not independent, as believed for nerve. Kinetically, TTX resembles local anesthetics, but its affinity remains unchanged during maintained depolarization. On this last point, comparison of our INa results and earlier upstroke velocity (Vmax) measurements illustrates how much these approaches can differ.     

T-type Ca2+ channel lowers the threshold of spike generation in the newt olfactory receptor cell

Mechanisms underlying action potential generation in the newt olfactory receptor cell were investigated by using the whole-cell version of the patch-clamp technique. Isolated olfactory cells had a resting membrane potential of -70 +/- 9 mV. Injection of a depolarizing current step triggered action potentials under current clamp condition. The amplitude of the action potential was reduced by lowering external Na+ concentration. After a complete removal of Na+, however, cells still showed action potentials which was abolished either by Ca2+ removal or by an application of Ca2+ channel blocker (Co2+ or Ni2+), indicating an involvement of Ca2+ current in spike generation of newt olfactory receptor cells. Under the voltage clamp condition, depolarization of the cell to -40 mV from the holding voltage of -100 mV induced a fast transient inward current, which consisted of Na+ (INa) and T-type Ca2+ (ICa.T) currents. The amplitude of ICa,T was about one fourth of that of INa. Depolarization to more positive voltages also induced L-type Ca2+ current (ICa,L). ICa,L was as small as a few pA in normal Ringer solution. The activating voltage of ICa,T was approximately 10 mV more negative than that of INa. Under current clamp, action potentials generated by a least effective depolarization was almost completely blocked by 0.1 mM Ni2+ (a specific T-type Ca2+ channel blocker) even in the presence of Na+. These results suggest that ICa,T contributes to action potential in the newt olfactory receptor cell and lowers the threshold of spike generation.     

Modification of inactivation in cardiac sodium channels: ionic current studies with Anthopleurin-A toxin

The site 3 toxin, Anthopleurin-A (Ap-A), was used to modify inactivation of sodium channels in voltage-clamped single canine cardiac Purkinje cells at approximately 12 degrees C. Although Ap-A toxin markedly prolonged decay of sodium current (INa) in response to step depolarizations, there was only a minor hyperpolarizing shift by 2.5 +/- 1.7 mV (n = 13) of the half-point of the peak conductance- voltage relationship with a slight steepening of the relationship from - 8.2 +/- 0.8 mV to -7.2 +/- 0.8 mV (n = 13). Increases in Gmax were dependent on the choice of cation used as a Na substitute intracellularly and ranged between 26 +/- 15% (Cs, n = 5) to 77 +/- 19% (TMA, n = 8). Associated with Ap-A toxin modification time to peak INa occurred later, but analysis of the time course INa at multiple potentials showed that the largest effects were on inactivation with only a small effect on activation. Consistent with little change in Na channel activation by Ap-A toxin, INa tail current relaxations at very negative potentials, where the dominant process of current relaxation is deactivation, were similar in control and after toxin modification. The time course of the development of inactivation after Ap-A toxin modification was dramatically prolonged at positive potentials where Na channels open. However, it was not prolonged after Ap-A toxin at negative potentials, where channels predominately inactivate directly from closed states. Steady state voltage-dependent availability (h infinity or steady state inactivation), which predominately reflects the voltage dependence of closed-closed transitions equilibrating with closed-inactivated transitions was shifted in the depolarizing direction by only 1.9 +/- 0.8 mV (n = 8) after toxin modification. The slope factor changed from 7.2 +/- 0.8 to 9.9 +/- 0.9 mV (n = 8), consistent with a prolongation of inactivation from the open state of Ap-A toxin modified channels at more depolarized potentials. We conclude that Ap-A selectively modifies Na channel inactivation from the open state with little effect on channel activation or on inactivation from closed state(s).     

Angiotensin II-induced stimulation of voltage-dependent Ca2+ currents in an adrenal cortical cell line.

Biochemical studies suggest that stimulation of aldosterone secretion by angiotensin II involves activation of voltage-dependent Ca2+ channels. We used an adrenocortical cell line (Y1) to study the effect of angiotensin II on transmembranous currents. The hormone (1 nM to 1 microM) caused depolarization of the plasma membrane (from -35 to 10 mV) and elicited repetitive action potentials. Using the whole-cell clamp technique, we identified two types of voltage-dependent Ca2+ currents which differed with respect to their threshold potential and time course of inactivation. Angiotensin II (1 nM to 1 microM) stimulated a slowly inactivating Ca2+ current on average up to 1.7-fold whereas a fast inactivating Ca2+ current remained almost unaffected by the hormone. Ca2+ currents were not influenced by forskolin (1 microM) or intracellularly applied cAMP (50 microM). Pretreatment of cells with pertussis toxin abolished the hormonal stimulation of the slowly inactivating Ca2+ current but was without effect on control currents. The toxin ADP-ribosylated a single membranous peptide of 40 kd Mr. An antiserum raised against a synthetic peptide corresponding to a region common to all sequenced alpha-subunits of guanine nucleotide-binding proteins (G-proteins) and an antiserum raised against a peptide corresponding to a region of alpha-subunits of Gi-like G-proteins reacted with membranous 40 kd peptides, whereas an antiserum raised against a synthetic peptide corresponding to a region specific for the alpha-subunit of the G-protein, G0, failed to recognize a peptide in the 39 to 40 kd region.(ABSTRACT TRUNCATED AT 250 WORDS)     

Comparison of the electrophysiological effect of amiodarone, lidocaine and quinidine on rat ventricular cells.

The effects of 20 microM each of amiodarone, lidocaine and quinidine on action potential and membrane currents were studied in rat ventricular cells. At a stimulation frequency of 0.1 Hz, quinidine prolonged the action potential duration (APD50) from 120 +/- 26 to 660 +/- 8 msec and increased the time to peak (Tp) amplitude from 7 +/- 1 msec to 32 +/- 6 msec. Lidocaine shortened APD50 from 123 +/- 15 to 83 +/- 6 msec without altering Tp. Amiodarone changed neither APD50 nor Tp. Voltage clamp study revealed that quinidine inhibited sodium inward current (INa) even when this current was elicited by depolarizing pulses at 0.1 Hz from a holding potential of -90 mV. For amiodarone and lidocaine, the inhibition was observed when INa was elicited from a holding potential of -70 mV. A frequency-dependent inhibition of INa by amiodarone and lidocaine was observed at frequencies higher than 1 Hz. Quinidine showed this inhibition even at 1 Hz. In correlation with the stronger frequency dependent inhibition of INa, a greater delay of the recovery and increase of the non-recovery fraction of INa was induced by quinidine. For lidocaine and amiodarone, only the recovery time constant was delayed. In cells treated with sea anemone toxin (ATX, 0.2 microM), APD50 was prolonged to 4-5 sec in 5 min. Quinidine, but not amiodarone, completely reversed the effect of ATX. Quinidine showed use-dependent inhibition of INa in these ATX-treated cells. Amiodarone, however, did not show this inhibition. It is likely that amiodarone suppresses INa by delaying the recovery of INa instead of blocking the open-state Na(+)-channels.(ABSTRACT TRUNCATED AT 250 WORDS)     

Ca(2+)-dependent inactivation of cardiac L-type Ca2+ channels does not affect their voltage sensor

Inactivation of currents carried by Ba2+ and Ca2+, as well as intramembrane charge movement from L-type Ca2+ channels were studied in guinea pig ventricular myocytes using the whole-cell patch clamp technique. Prolonged (2 s) conditioning depolarization caused substantial reduction of charge movement between -70 and 10 mV (charge 1, or charge from noninactivated channels). In parallel, the charge mobile between -70 and -150 mV (charge 2, or charge from inactivated channels) was increased. The availability of charge 2 depended on the conditioning pulse voltage as the sum of two Boltzmann components. One component had a central voltage of -75 mV and a magnitude of 1.7 nC/microF. It presumably is the charge movement (charge 2) from Na+ channels. The other component, with a central voltage of approximately - 30 mV and a magnitude of 3.5 nC/microF, is the charge 2 of L-type Ca2+ channels. The sum of charge 1 and charge 2 was conserved after different conditioning pulses. The difference between the voltage dependence of the activation of L-type Ca2+ channels (half-activation voltage, V, of approximately -20 mV) and that of charge 2 (V of -100 mV) made it possible to record the ionic currents through Ca2+ channels and charge 2 in the same solution. In an external solution with Ba2+ as sole metal the maximum available charge 2 of L-type Ca2+ channels was 10-15% greater than that in a Ca(2+)-containing solution. External Cd2+ caused 20-30% reduction of charge 2 both from Na+ and L-type Ca2+ channels. Voltage- and Ca(2+)-dependent inactivation phenomena were compared with a double pulse protocol in cells perfused with an internal solution of low calcium buffering capacity. As the conditioning pulse voltage increased, inactivation monitored with the second pulse went through a minimum at about 0 mV, the voltage at which conditioning current had its maximum. Charge 2, recorded in parallel, did not show any increase associated with calcium entry. Two alternative interpretations of these observations are: (a) that Ca(2+)- dependent inactivation does not alter the voltage sensor, and (b) that inactivation affects the voltage sensor, but only in the small fraction of channels that open, and the effect goes undetected. A model of channel gating that assumes the first possibility is shown to account fully for the experimental results. Thus, extracellular divalent cations modulate voltage-dependent inactivation of the Ca2+ channel. Intracellular Ca2+ instead, appears to cause inactivation of the channel without affecting its voltage sensor.     

Voltage-dependent inactivation of slow calcium channels in intact twitch muscle fibers of the frog

Inactivation of slow Ca2+ channels was studied in intact twitch skeletal muscle fibers of the frog by using the three-microelectrode voltage-clamp technique. Hypertonic sucrose solutions were used to abolish contraction. The rate constant of decay of the slow Ca2+ current (ICa) remained practically unchanged when the recording solution containing 10 mM Ca2+ was replaced by a Ca2+-buffered solution (126 mM Ca-maleate). The rate constant of decay of ICa monotonically increased with depolarization although the corresponding time integral of ICa followed a bell-shaped function. The replacement of Ca2+ by Ba2+ did not result in a slowing of the rate of decay of the inward current nor did it reduce the degree of steady-state inactivation. The voltage dependence of the steady-state inactivation curve was steeper in the presence of Ba2+. In two-pulse experiments with large conditioning depolarizations ICa inactivation remained unchanged although Ca2+ influx during the prepulse greatly decreased. Dantrolene (12 microM) increased mechanical threshold at all pulse durations tested, the effect being more prominent for short pulses. Dantrolene did not significantly modify ICa decay and the voltage dependence of inactivation. These results indicate that in intact muscle fibers Ca2+ channels inactivate in a voltage-dependent manner through a mechanism that does not require Ca2+ entry into the cell.     

Activation-inactivation coupling in Myxicola giant axons injected with tetraethylammonium.

Myxicola giant axons internally injected with tetraethylammonium chloride to block potassium currents were examined under voltage clamp. The sodium inactivation time constants obtained from the decline in INa during step depolarizations were substantially smaller than those obtained using conditioning prepulses to the same potentials and the ratios agreed with previous observations using TTX. Inactivation shifts were also measured and found to be comparable to previous results.     

The Mu class glutathione transferase is abundant in striated muscle and is an isoform-specific regulator of ryanodine receptor calcium channels

Members of the glutathione transferase (GST) structural family are novel regulators of cardiac ryanodine receptor (RyR) calcium channels. We present the first detailed report of the effect of endogenous muscle GST on skeletal and cardiac RyRs. An Mu class glutathione transferase is specifically expressed in human muscle. An hGSTM2-2-like protein was isolated from rabbit skeletal muscle and sheep heart, at concentrations of approximately 17-93 microM. When added to the cytoplasmic side of RyRs, hGSTM2-2 and GST isolated from skeletal or cardiac muscle, modified channel activity in an RyR isoform-specific manner. High activity skeletal RyR1 channels were inactivated at positive potentials or activated at negative potentials by hGSTM2-2 (8-30 microM). Inactivation became faster as the positive voltage was increased. Channels recovered from inactivation when the voltage was reversed, but recovery times were significantly slowed in the presence of hGSTM2-2 and muscle GSTs. Low activity RyR1 channels were activated at both potentials. In contrast, hGSTM2-2 and GSTs isolated from muscle (1-30 microM) in the cytoplasmic solution, caused a voltage-independent inhibition of cardiac RyR2 channels. The results suggest that the major GST isoform expressed in muscle regulates Ca2+ signalling in skeletal and cardiac muscle and conserves Ca2+ stores in the sarcoplasmic reticulum.     

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.     

Voltage-clamp of cut-end skeletal muscle fibre: a diffusion experiment

Membrane potential and current were studied in cut end fibres of frog skeletal muscle under current and voltage clamp conditions, by the double sucrose gap technique. Similar action potentials were recorded under current clamp conditions with either the microelectrode or the double sucrose gap techniques. Under voltage clamp conditions, the control of the membrane potential was maintained adequately. The early current was sensitive to both TTX and external Na concentration suggesting that the current was carried by Na ions. Sodium current (INa) was subsequently analysed using the Hodgkin-Huxley formulae. INa half-activation and inactivation occurred at -34 mV and -60 mV, respectively. Na-rich solution applied internally by diffusion through cut ends produced a reduction of INa associated with a shift of the sodium current reversal potential (VNa) towards more negative membrane potentials. This suggested that the sodium electromotive force was reduced by the increase in internal Na content of the fibre. Iodate applied externally changed neither the activation nor the inactivation time courses of INa, but reduced the peak current. Conversely, internally applied by diffusion from the cut end of skeletal muscle fibre, iodate slowed down the time course of INa inactivation and decreased the current peak. In conclusion, the double sucrose gap technique adapted to cut end frog skeletal muscle fibre allows a satisfactory analysis of INa.     

Aluminum enhances the voltage activated sodium currents in the neurons of the pond snail Lymnaea stagnalis L

1. The effects of aluminum on voltage activated sodium currents (VASCs) were investigated by using the conventional two-electrode voltage clamp technique in Lymnaea stagnalis L. neurons. The peak amplitude, kinetics, and voltage-dependence of activation and inactivation of the sodium currents were studied in the presence of 5-500 microM AlCl3, at pH = 7.7. 2. There was a significant concentration-dependent increase in the peak amplitude of sodium currents after Al treatment, ED50 = 67 microM. The threshold concentration of the enhancement was 50 microM. The maximal peak increase of 143% was caused by a 500 microM aluminum. The action of aluminum on VASCs developed slowly, and it is not recovered by washing within 20 min. 3. There was little alteration of the voltage-dependence of the current. It was not a significant effect on the activation- and inactivation time constants of INa, but the steady-state inactivation curve shifted to negative direction on the voltage axis in the presence of Al. 4. The leak currents were not influenced by aluminum up to the highest concentration applied.     

Bethanidine increased Na+ and Ca2+ currents and caused a positive inotropic effect in heart cells

The effects of bethanidine sulphate, a pharmacological analog of the cardiac antibrillatory drug, bretylium tosylate, were studied on action potentials (APs) and K+, Na+, and Ca2+ currents of single cultured embryonic chick heart cells using the whole-cell current clamp and voltage clamp technique. Extracellular application of bethanidine (3 X 10(-4) M) increased the overshoot and the duration of the APs and greatly decreased the outward K+ current (IK) and potentiated the inward fast Na+ currents (INa) and the inward slow calcium current (ICa). However, intracellular introduction of bethanidine (10(-4) M) blocked INa. In isolated atria of rat, bethanidine increased the force of contraction in a dose-dependent manner. These findings suggest that when applied extracellularly, bethanidine exerts a potentiating effect on the myocardial fast Na+ current and slow Ca2+ current and an inhibitory effect of IK. The positive inotropic effect of bethanidine could be due, at least in part, to an increase of Ca2+ influx via the slow Ca2+ channel and the Na-Ca exchange. It is suggested that the decrease of IK by bethanidine may account for its antifibrillatory action.     

The protein kinase C inhibitor, bisindolylmaleimide (I), inhibits voltage-dependent K+ channels in coronary arterial smooth muscle cells

We examined the effects of the protein kinase C (PKC) inhibitor, bisindolylmaleimide (BIM) (I), on voltage-dependent K+ (K(V)) channels in rabbit coronary arterial smooth muscle cells using whole-cell patch clamp technique. BIM (I) reversibly and dose-dependently inhibited the K(V) currents with an apparent Kd value of 0.27 microM. The inhibition of the K(V) current by BIM (I) was highly voltage-dependent between -30 and +10 mV (voltage range of channel activation), and the additive inhibition of the K(V) current by BIM (I) was voltage-dependence in the full activation voltage range. The rate constants of association and dissociation for BIM (I) were 18.4 microM(-1) s(-1) and 4.7 s(-1), respectively. BIM (I) had no effect on the steady-state activation and inactivation of K(V) channels. BIM (I) caused use-dependent inhibition of K(V) current, which was consistent with the slow recovery from inactivation in the presence of BIM (I) (recovery time constants were 856.95 +/- 282.6 ms for control, and 1806.38 +/- 110.0 ms for 300 nM BIM (I)). ATP-sensitive K+ (K(ATP)), inward rectifier K+ (K(IR)), Ca2+-activated K+ (BK(Ca)) channels, which regulate the membrane potential and arterial tone, were not affected by BIM (I). The PKC inhibitor, chelerythrine, and protein kinase A (PKA) inhibitor, PKA-IP, had little effect on the K(V) current and did not significantly alter the inhibitory effects of BIM (I) on the K(V) current. These results suggest that BIM (I) inhibits K(V) channels in a phosphorylation-independent, and voltage-, time- and use-dependent manner.     

Calcium currents in the A7r5 smooth muscle-derived cell line. Calcium- dependent and voltage-dependent inactivation

Inactivation of a dihydropyridine-sensitive calcium current was studied in a cell line (A7r5) derived from smooth muscle of the rat thoracic aorta. Inactivation is faster with extracellular Ca2+ than with Ba2+. In Ba2+, inactivation increases monotonically with depolarization. In Ca2+, inactivation is related to the amount of inward current, so that little inactivation is seen in Ca2+ for brief depolarizations approaching the reversal potential. Longer depolarizations in Ca2+ reveal two components of inactivation, the slower component behaving like that observed in Ba2+. Furthermore, lowering extracellular Ca2+ slows inactivation. These results are consistent with the coexistence of two inactivation processes, a slow voltage-dependent inactivation, and a more rapid current-dependent inactivation which is observable only with Ca2+. Ca(2+)-dependent inactivation is decreased but not eliminated when intracellular Ca2+ is buffered by 10 mM BAPTA, suggesting that Ca2+ acts at a site on or near the channel. We also studied recovery from inactivation after either a short pulse (able to produce significant inactivation only in Ca2+) or a long pulse (giving similar inactivation with either cation). Surprisingly, recovery from Ca(2+)-dependent inactivation was voltage dependent. This suggests that the pathways for recovery from inactivation are similar regardless of how inactivation is generated. We propose a model where Ca(2+)- and voltage-dependent inactivation occur independently.     

Bunazosin, an alpha-adrenoceptor antagonist, blocks calcium current in guinea-pig ventricular myocytes.

1. Effect of bunazosin, an alpha 1-adrenoceptor antagonist, upon the slow inward Ca2+ current (ICa) was studied in single ventricular myocytes of the guinea-pig using a whole-cell patch-clamp technique. 2. Bunazosin (10-100 microM) decreased ICa in a concentration-dependent manner with an IC50 of 60 microM during depolarization to + 10 mV from the holding potential of -40 mV. 3. As for the inactivation process of ICa, the steady-state inactivation (f infinity) curve was shifted toward more negative potentials from -12 mV to -17 mV and -21 mV at f infinity = 0.5, by 30 microM and 70 microM bunazosin. 4. Inhibition of ICa by the compound (10 microM) was also dependent on stimulation frequency, with greater block induced at 2 Hz (50%) than at 0.33 Hz (13%). 5. It is concluded that bunazosin possesses a direct Ca2+ channel-blocking (class 4) action in a rate-dependent fashion.     

Slow inactivation and reactivation of the K+ channel in squid axons. A tail current analysis.

Potassium current inactivation and reactivation in squid axons were measured from tail current amplitudes after voltage clamp prepulses to the potassium equilibrium potential, EK, in seawater containing elevated levels of potassium ion concentration, Ko. Little or no inactivation resulted with prepulses lasting less than 100 ms. Longer pulses caused the current to inactivate in two phases, one between 0.1 and 1 s, and a second phase between 5 and 100 s. Inactivation was incomplete. The time constant of the tail current after a prepulse to EK was independent of pulse duration (0.1-120 s). Inactivation was independent of Ko (10 less than or equal to Ko less than or equal to 300 mM), and it was independent of membrane potential, V, for -40 less than or equal to V less than or equal to 0 mV. Reactivation was measured with a three-pulse protocol. The reactivation time course was sigmoidal with a delay of approximately 100 ms before significant reactivation occurred. These results were described by a model consisting of three inactivated states arranged in a linear sequence. The rate constants of the model are of the form (A + B exp (CV), or 1/(A + B exp (CV], which are required to describe the non-inactivating conductance component.