Fast and slow voltage sensor movements in HERG potassium channels

HERG encodes an inwardly-rectifying potassium channel that plays an important role in repolarization of the cardiac action potential. Inward rectification of HERG channels results from rapid and voltage-dependent inactivation gating, combined with very slow activation gating. We asked whether the voltage sensor is implicated in the unusual properties of HERG gating: does the voltage sensor move slowly to account for slow activation and deactivation, or could the voltage sensor move rapidly to account for the rapid kinetics and intrinsic voltage dependence of inactivation? To probe voltage sensor movement, we used a fluorescence technique to examine conformational changes near the positively charged S4 region. Fluorescent probes attached to three different residues on the NH₂-terminal end of the S4 region (E518C, E519C, and L520C) reported both fast and slow voltage-dependent changes in fluorescence. The slow changes in fluorescence correlated strongly with activation gating, suggesting that the slow activation gating of HERG results from slow voltage sensor movement. The fast changes in fluorescence showed voltage dependence and kinetics similar to inactivation gating, though these fluorescence signals were not affected by external tetraethylammonium blockade or mutations that alter inactivation. A working model with two types of voltage sensor movement is proposed as a framework for understanding HERG channel gating and the fluorescence signals.     

A high-Na(+) conduction state during recovery from inactivation in the K(+) channel Kv1.5

Na(+) conductance through cloned K(+) channels has previously allowed characterization of inactivation and K(+) binding within the pore, and here we have used Na(+) permeation to study recovery from C-type inactivation in human Kv1.5 channels. Replacing K(+) in the solutions with Na(+) allows complete Kv1.5 inactivation and alters the recovery. The inactivated state is nonconducting for K(+) but has a Na(+) conductance of 13% of the open state. During recovery, inactivated channels progress to a higher Na(+) conductance state (R) in a voltage-dependent manner before deactivating to closed-inactivated states. Channels finally recover from inactivation in the closed configuration. In the R state channels can be reactivated and exhibit supernormal Na(+) currents with a slow biexponential inactivation. Results suggest two pathways for entry to the inactivated state and a pore conformation, perhaps with a higher Na(+) affinity than the open state. The rate of recovery from inactivation is modulated by Na(+)(o) such that 135 mM Na(+)(o) promotes the recovery to normal closed, rather than closed-inactivated states. A kinetic model of recovery that assumes a highly Na(+)-permeable state and deactivation to closed-inactivated and normal closed states at negative voltages can account for the results. Thus these data offer insight into how Kv1. 5 channels recover their resting conformation after inactivation and how ionic conditions can modify recovery rates and pathways.     

Uncoupling of gating charge movement and closure of the ion pore during recovery from inactivation in the Kv1.5 channel

Both wild-type (WT) and nonconducting W472F mutant (NCM) Kv1.5 channels are able to conduct Na(+) in their inactivated states when K(+) is absent. Replacement of K(+) with Na(+) or NMG(+) allows rapid and complete inactivation in both WT and W472F mutant channels upon depolarization, and on return to negative potentials, transition of inactivated channels to closed-inactivated states is the first step in the recovery of the channels from inactivation. The time constant for immobilized gating charge recovery at -100 mV was 11.1 +/- 0.4 ms (n = 10) and increased to 19.0 +/- 1.6 ms (n = 3) when NMG(+)(o) was replaced by Na(+)(o). However, the decay of the Na(+) tail currents through inactivated channels at -100 mV had a time constant of 129 +/- 26 ms (n = 18), much slower than the time required for gating charge recovery. Further experiments revealed that the voltage-dependence of gating charge recovery and of the decay of Na(+) tail currents did not match over a 60 mV range of repolarization potentials. A faster recovery of gating charge than pore closure was also observed in WT Kv1.5 channels. These results provide evidence that the recovery of the gating elements is uncoupled from that of the pore in Na(+)-conducting inactivated channels. The dissociation of the gating charge movements and the pore closure could also be observed in the presence of symmetrical Na(+) but not symmetrical Cs(+). This difference probably stems from the difference in the respective abilities of the two ions to limit inactivation to the P-type state or prevent it altogether.     

Time- and voltage-dependent components of Kv4.3 inactivation

Kv4.3 inactivation is a complex multiexponential process, which can occur from both closed and open states. The fast component of inactivation is modulated by the N-terminus, but the mechanisms mediating the other components of inactivation are controversial. We studied inactivation of Kv4.3 expressed in Xenopus laevis oocytes, using the two-electrode voltage-clamp technique. Inactivation during 2000 ms pulses at potentials positive to the activation threshold was described by three exponents (46 +/- 3, 152 +/- 13, and 930 +/- 50 ms at +50 mV, n = 7) whereas closed-state inactivation (at potentials below threshold) was described by two exponents (1079 +/- 119 and 3719 +/- 307 ms at -40 mV, n = 9). The fast component of open-state inactivation was dominant at potentials positive to -20 mV. Negative to -30 mV, the intermediate and slow components dominated inactivation. Inactivation properties were dependent on pulse duration. Recovery from inactivation was strongly dependent on voltage and pulse duration. We developed an 11-state Markov model of Kv4.3 gating that incorporated a direct transition from the open-inactivated state to the closed-inactivated state. Simulations with this model reproduced open- and closed-state inactivation, isochronal inactivation relationships, and reopening currents. Our data suggest that inactivation can proceed primarily from the open state and that multiple inactivation components can be identified.     

Regulation of Deactivation by an Amino Terminal Domain in Human Ether-à-go-go?–related Gene Potassium Channels

Abnormalities in repolarization of the cardiac ventricular action potential can lead to life-threatening arrhythmias associated with long QT syndrome. The repolarization process depends upon the gating properties of potassium channels encoded by the human ether-à-go-go–related gene (HERG), especially those governing the rate of recovery from inactivation and the rate of deactivation. Previous studies have demonstrated that deletion of the NH₂ terminus increases the deactivation rate, but the mechanism by which the NH₂ terminus regulates deactivation in wild-type channels has not been elucidated. We tested the hypothesis that the HERG NH₂ terminus slows deactivation by a mechanism similar to N-type inactivation in Shaker channels, where it binds to the internal mouth of the pore and prevents channel closure. We found that the regulation of deactivation by the HERG NH₂ terminus bears similarity to Shaker N-type inactivation in three respects: (a) deletion of the NH₂ terminus slows C-type inactivation; (b) the action of the NH₂ terminus is sensitive to elevated concentrations of external K⁺, as if its binding along the permeation pathway is disrupted by K⁺ influx; and (c) N-ethylmaleimide, covalently linked to an aphenotypic cysteine introduced within the S4–S5 linker, mimics the N deletion phenotype, as if the binding of the NH₂ terminus to its receptor site were hindered. In contrast to N-type inactivation in Shaker, however, there was no indication that the NH₂ terminus blocks the HERG pore. In addition, we discovered that separate domains within the NH₂ terminus mediate the slowing of deactivation and the promotion of C-type inactivation. These results suggest that the NH₂ terminus stabilizes the open state and, by a separate mechanism, promotes C-type inactivation.     

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

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

Enhancement of HERG K(+) currents by Cd(2+) destabilization of the inactivated state

We have studied the functional effects of extracellular Cd(2+) on human ether-a-go-go-related gene (HERG) encoded K(+) channels. Low concentrations (10-200 &mgr;M) of extracellular Cd(2+) increased outward currents through HERG channels; 200 &mgr;M Cd(2+) more than doubled HERG currents and altered current kinetics. Cd(2+) concentrations up to 200 &mgr;M did not change the voltage dependence of channel activation, but shifted the voltage dependence of inactivation to more depolarized membrane potentials. Cd(2+) concentrations >/=500 &mgr;M shifted the voltage dependence of channel activation to more positive potentials. These results are consistent with a somewhat specific ability of Cd(2+) to destabilize the inactivated state. We tested the hypothesis that channel inactivation is essential for Cd(2+)-induced increases in HERG K(+) currents, using a double point mutation (G628C/S631C) that diminishes HERG inactivation (Smith, P. L., T. Baukrowitz, and G. Yellen. 1996. Nature (Lond.). 379:833-836). This inactivation-removed mutant is insensitive to low concentrations of Cd(2+). Thus, Cd(2+) had two distinct effects on HERG K(+) channels. Low concentrations of Cd(2+) caused relatively selective effects on inactivation, resulting in a reduction of the apparent rectification of the channel and thereby increasing HERG K(+) currents. Higher Cd(2+) concentrations affected activation gating as well, possibly by a surface charge screening mechanism or by association with a lower affinity site.     

Expression and Functional Characterization of the Human Ether-à-go-go-Related Gene (<Emphasis Type="Italic">HERG</Emphasis>) K<Superscript>+</Superscript> Channel Cardiac Splice Variant in <Emphasis Type="Italic">Xenopus laevis</Emphasis> Oocytes

HERG C_Cardiac, a C-terminal splice variant of the human ether-à-go-go-related gene (HERG A), was identified and found to be 100% homologous to HERG_USO. Real-time polymerase chain reaction data indicated that in the human heart HERG C_Cardiac mRNA was expressed eight times more than HERG A, whereas in human ventricular tissue it was expressed six times more than HERG A. A HERG C_Cardiac-green fluorescence protein (GFP) construct was heterologously expressed in Xenopus oocytes. Confocal micrographs revealed that HERG C_Cardiac was mainly expressed in the plasma membrane. HERG C_Cardiac channel expressed in oocytes produced slower inactivating outward currents and faster deactivating tail currents than those of HERG A channel. Equal amounts of HERG A and HERG C_Cardiac cRNA coinjected into oocytes formed intermediate HERG A + HERG C_Cardiac heteromultimers, which was reconfirmed by immunoprecipitation experiments with a HERG A N-terminal antibody. These heteromultimers had different inactivation, deactivation and activation kinetics from those of HERG A and HERG C_Cardiac channels. HERG A + HERG C_Cardiac heteromultimers significantly reduced the model action potential mean amplitude and increased the fast and slow inactivation τ values of the action potential repolarization phase, suggesting involvement of HERG A and HERG C_Cardiac heteromultimers in modulation of the refractory interval.     

Na+ permeation and block of hERG potassium channels

The inactivation gating of hERG channels is important for the channel function and drug-channel interaction. Whereas hERG channels are highly selective for K+, we have found that inactivated hERG channels allow Na+ to permeate in the absence of K+. This provides a new way to directly monitor and investigate hERG inactivation. By using whole cell patch clamp method with an internal solution containing 135 mM Na+ and an external solution containing 135 mM NMG+, we recorded a robust Na+ current through hERG channels expressed in HEK 293 cells. Kinetic analyses of the hERG Na+ and K+ currents indicate that the channel experiences at least two states during the inactivation process, an initial fast, less stable state followed by a slow, more stable state. The Na+ current reflects Na+ ions permeating through the fast inactivated state but not through the slow inactivated state or open state. Thus the hERG Na+ current displayed a slow inactivation as the channels travel from the less stable, fast inactivated state into the more stable, slow inactivated state. Removal of fast inactivation by the S631A mutation abolished the Na+ current. Moreover, acceleration of fast inactivation by mutations T623A, F627Y, and S641A did not affect the hERG Na+ current, but greatly diminished the hERG K+ current. We also found that external Na+ potently blocked the hERG outward Na+ current with an IC50 of 3.5 mM. Mutations in the channel pore and S6 regions, such as S624A, F627Y, and S641A, abolished the inhibitory effects of external Na+ on the hERG Na+ current. Na+ permeation and blockade of hERG channels provide novel ways to extend our understanding of the hERG gating mechanisms.     

Upregulation of HERG channels by the serum and glucocorticoid inducible kinase isoform SGK3.

Human ether-a-go-go (HERG) channels participate in the repolarization of the cardiac action potential. Loss of function mutations of HERG lead to delayed cardiac repolarization reflected by prolonged QT interval. HERG channels are regulated through a signaling cascade involving phosphatidylinositol 3 (PI3) kinase. Downstream targets of PI3 kinase include the serum and glucocorticoid inducible kinase (SGK) and protein kinase B (PKB) isoforms. The present study has been performed to explore whether SGK1 and SGK3 participate in the regulation of HERG channel activity. HERG was expressed in Xenopus oocytes with or without additional expression of SGK1 or SGK3. Chemiluminescence was employed to determine HERG plasma membrane protein abundance. Coexpression of SGK3 but not of SGK1 in Xenopus oocytes resulted in an increase of steady state current (I(HERG)) and enhanced cell membrane protein abundance without affecting gating kinetics of the channel. Replacement of serine by alanine at the two SGK consensus sites decreased I(HERG) but neither mutation abolished the stimulating effect of SGK3. In conclusion, SGK3 participates in the regulation of HERG by increasing HERG protein abundance in the plasma membrane and may thus modify the duration of the cardiac action potential.     

Anomalous L-type calcium channels of rat spinal motoneurons

Single channel patch-clamp recordings show that embryonic rat spinal motoneurons express anomalous L-type calcium channels, which reopen upon repolarization to resting potentials, displaying both short and long reopenings. The probability of reopening increases with increasing voltage of the preceding depolarization without any apparent correlation with inactivation during the depolarization. The probability of long with respect to short reopenings increases with increasing length of the depolarization, with little change in the total number of reopenings and in their delay. With less negative repolarization voltages, the delay increases, while the mean duration of both short and long reopenings decreases, remaining longer than that of the openings during the preceding depolarization. Open times decrease with increasing voltage in the range -60 to +40 mV. Closed times tend to increase at V > 20 mV. The open probability is low at all voltages and has an anomalous bell-shaped voltage dependence. We provide evidence that short and long reopenings of anomalous L-type channels correspond to two gating modes, whose relative probability depends on voltage. Positive voltages favor both the transition from a short-opening to a long-opening mode and the occupancy of a closed state outside the activation pathway within each mode from which the channel reopens upon repolarization. The voltage dependence of the probability of reopenings reflects the voltage dependence of the occupancy of these closed states, while the relative probability of long with respect to short reopenings reflects the voltage dependence of the equilibrium between modes. The anomalous gating persists after patch excision, and therefore our data rule out voltage-dependent block by diffusible ions as the basis for the anomalous gating and imply that a diffusible cytosolic factor is not necessary for voltage-dependent potentiation of anomalous L-type channels.     

New Aspects of HERG K+ Channel Function Depending upon Cardiac Spatial Heterogeneity

HERG K⁺ channel, the genetic counterpart of rapid delayed rectifier K⁺ current in cardiac cells, is responsible for many cases of inherited and drug-induced long QT syndromes. HERG has unusual biophysical properties distinct from those of other K⁺ channels. While the conventional pulse protocols in patch-clamp studies have helped us elucidate these properties, their limitations in assessing HERG function have also been progressively noticed. We employed AP-clamp techniques using physiological action potential waveforms recorded from various regions of canine heart to study HERG function in HEK293 cells and identified several novel aspects of HERG function. We showed that under AP-clamp I_HERG increased gradually with membrane repolarization, peaked at potentials around 20–30 mV more negative than revealed by pulse protocols and at action potential duration (APD) to 60%-70% full repolarization, and fell rapidly at the terminal phase of repolarization. We found that the rising phase of I_HERG was conferred by removal of inactivation and the decaying phase resulted from a fall in driving force, which were all determined by the rate of membrane repolarization. We identified regional heterogeneity and transmural gradient of I_HERG when quantified with the area covered by I_HERG trace. In addition, we observed regional and transmural differences of I_HERG in response to dofetilide blockade. Finally, we characterized the influence of HERG function by selective inhibition of other ion currents. Based on our results, we conclude that the distinct biophysical properties of HERG reported by AP-clamp confer its unique function in cardiac repolarization thereby in antiarrhythmia and arrhythmogenesis.     

Shaker IR T449 Mutants Separate C- from U-Type Inactivation

Previous studies demonstrated that slow inactivation of the Shaker potassium channel can be made ~100-fold faster or slower by point mutations at a site in the outer pore (T449). However, the discovery that two forms of slow inactivation coexist in Shaker raises the question of which inactivation process is affected by mutation. Equivalent mutations in K_V2.1, a channel exhibiting only U-type inactivation, have minimal effects on inactivation, suggesting that mutation of Shaker T449 acts on C-type inactivation alone, a widely held yet untested hypothesis. This study reexamines mutations at Shaker T449, confirming that T449A speeds inactivation and T449Y/V slow it. T449Y and T449V exhibit U-type inactivation that is enhanced by high extracellular potassium, in contrast to C-type inactivation in T449A which is inhibited by high potassium. Automated parameter estimation for a 12-state Markov model suggests that U-type inactivation occurs mainly from closed states upon weak depolarization, but primarily from the open state at positive voltages. The model also suggests that WT channels, which in this study exhibit mostly C-type inactivation, recover from inactivation through closed-inactivated states, producing voltage-dependent recovery. This suggests that both C-type and U-type inactivation involve both open-inactivated and closed-inactivated states.     

Modulation of HERG gating by a charge cluster in the N-terminal proximal domain

Human ether-a-go-go-related gene (HERG) potassium channels contribute to the repolarization of the cardiac action potential and display unique gating properties with slow activation and fast inactivation kinetics. Deletions in the N-terminal 'proximal' domain (residues 135-366) have been shown to induce hyperpolarizing shifts in the voltage dependence of activation, suggesting that it modulates activation. However, we did not observe a hyperpolarizing shift with a subtotal deletion designed to preserve the local charge distribution, and other deletions narrowed the region to the KIKER containing sequence 362-372. Replacing the positively charged residues of this sequence by negative ones (EIEEE) resulted in a -45 mV shift of the voltage dependence of activation. The shifts were intermediate for individual charge reversals, whereas E365R resulted in a positive shift. Furthermore, the shifts in the voltage dependence were strongly correlated with the net charge of the KIKER region. The apparent speeding of the activation was attributable to the shifted voltage dependence of activation. Additionally, the introduction of negative charges accelerated the intermediate voltage-independent forward rate constant. We propose that the modulatory effects of the proximal domain on HERG gating are largely electrostatic, localized to the charged KIKER sequence.     

Gating of cardiac Na+ channels in excised membrane patches after modification by alpha-chymotrypsin.

Single cardiac Na+ channels were investigated after intracellular proteolysis to remove the fast inactivation process in an attempt to elucidate the mechanisms of channel gating and the role of slow inactivation. Na+ channels were studied in inside-out patches excised from guinea-pig ventricular myocytes both before and after very brief exposure (2-4 min) to the endopeptidase, alpha-chymotrypsin. Enzyme exposure times were chosen to maximize removal of fast inactivation and to minimize potential nonspecific damage to the channel. After proteolysis, the single channel current-voltage relationship was approximately linear with a slope conductance of 18 +/- 2.5 pS. Na+ channel reversal potentials measured before and after proteolysis by alpha-chymotrypsin were not changed. The unitary current amplitude was not altered after channel modification suggesting little or no effect on channel conductance. Channel open times were increased after removal of fast inactivation and were voltage-dependent, ranging between 0.7 (-70 mV) and 3.2 (-10 mV) ms. Open times increased with membrane potential reaching a maximum at -10 mV; at more positive membrane potentials, open times decreased again. Fast inactivation appeared to be completely removed by alpha-chymotrypsin and slow inactivation became more apparent suggesting that fast and slow inactivation normally compete, and that fast inactivation dominates in unmodified channels. This finding is not consistent with a slow inactivated state that can only be entered through the fast inactivated state, since removal of fast inactivation does not eliminate slow inactivation. The data indicate that cardiac Na+ channels can enter the slow inactivated state by a pathway that bypasses the fast inactivated state and that the likelihood of entering the slow inactivated state increases after removal of fast inactivation.     

Cooperative interactions between R531 and acidic residues in the voltage sensing module of hERG1 channels.

HERG1 K(+) channels are critical for modulating the duration of the cardiac action potential. The role of hERG1 channels in maintaining electrical stability in the heart derives from their unusual gating properties: slow activation and fast inactivation. HERG1 channel inactivation is intrinsically voltage sensitive and is not coupled to activation in the same way as in the Shaker family of K(+) channels. We recently proposed that the S4 transmembrane domain functions as the primary voltage sensor for hERG1 activation and inactivation and that distinct regions of S4 contribute to each gating process. In this study, we tested the hypothesis that S4 rearrangements underlying activation and inactivation gating may be associated with distinct cooperative interactions between a key residue in the S4 domain (R531) and acidic residues in neighboring regions (S1 - S3 domains) of the voltage sensing module. Using double-mutant cycle analysis, we found that R531 was energetically coupled to all acidic residues in S1-S3 during activation, but was coupled only to acidic residues near the extracellular portion of S2 and S3 (D456, D460 and D509) during inactivation. We propose that hERG1 activation involves a cooperative conformational change involving the entire voltage sensing module, while inactivation may involve a more limited interaction between R531 and D456, D460 and D509.     

Reopening of Ca2+ channels in mouse cerebellar neurons at resting membrane potentials during recovery from inactivation.

Recordings of single-channel activity from cerebellar granule cells show that a component of Ca2+ entry flows through L-type Ca2+ channels that are closed at negative membrane potentials following a strong depolarization, but then open after a delay. The delayed openings can be explained if membrane depolarization drives Ca2+ channels into an inactivated state and some channels return to rest through the open state after repolarization. Whole-cell recordings show that the charge carried by Ca2+ during the tail increases as inactivation progresses, whereas the current during the voltage step decreases. Voltage-dependent inactivation may be a general mechanism in central neurons for enhancing Ca2+ entry by delaying it until after repolarization, when the driving force for ion entry is large. Modifying the rate and extent of inactivation would have large effects on Ca2+ entry through those channels that recover from inactivation by passing through the open state.     

Molecular Analysis of the Putative Inactivation Particle in the Inactivation Gate of Brain Type IIA Na+ Channels

Fast Na⁺ channel inactivation is thought to involve binding of phenylalanine 1489 in the hydrophobic cluster IFM in L_III-IV of the rat brain type IIA Na⁺ channel. We have analyzed macroscopic and single channel currents from Na⁺ channels with mutations within and adjacent to hydrophobic clusters in L_III-IV. Substitution of F1489 by a series of amino acids disrupted inactivation to different extents. The degree of disruption was closely correlated with the hydrophilicity of the amino acid at position 1489. These mutations dramatically destabilized the inactivated state and also significantly slowed the entry into the inactivated state, consistent with the idea that F1489 forms a hydrophobic interaction with a putative receptor during the fast inactivation process. Substitution of a phe residue at position 1488 or 1490 in mutants lacking F1489 did not restore normal inactivation, indicating that precise location of F1489 is critical for its function. Mutations of T1491 disrupted inactivation substantially, with large effects on the stability of the inactivated state and smaller effects on the rate of entry into the inactivated state. Mutations of several other hydrophobic residues did not destabilize the inactivated state at depolarized potentials, indicating that the effects of mutations at F1489 and T1491 are specific. The double mutant YY1497/8QQ slowed macroscopic inactivation at all potentials and accelerated recovery from inactivation at negative membrane potentials. Some of these mutations in L_III-IV also affected the latency to first opening, indicating coupling between L_III-IV and channel activation. Our results show that the amino acid residues of the IFM hydrophobic cluster and the adjacent T1491 are unique in contributing to the stability of the inactivated state, consistent with the designation of these residues as components of the inactivation particle responsible for fast inactivation of Na⁺ channels.     

Redox state dependency of HERGS631C channel pharmacology: relation to C-type inactivation

The S631C mutation in human ether-à-go-go-related gene (HERG) channels has previously been reported to disrupt C-type inactivation and ion-selectivity when Cys-631 is in the oxidized state. In this study, we report the relation between pharmacology and C-type inactivation for HERGS631C channels. We demonstrate that HERGS631C in its reduced state is fully blocked by 1 microM astemizole, terfenadine and dofetilide, similar to wild-type HERG channels. In contrast, oxidized HERGS631C is insensitive for these blockers. Our results suggest that an interaction with HERG channels in the inactivated state might be a common mechanism to a variety of drugs known to block HERG channels with high affinity.     

Zn(2+) modulation of neuronal transient K(+) current: fast and selective binding to the deactivated channels

Modulation of voltage-dependent transient K(+) currents (A type K(+) or K(A) current) by Zn(2+) was studied in rat hippocampal neurons by the whole-cell patch-clamp technique. It is found that Zn(2+) selectively binds to the resting (deactivated or closed) K(A) channels with a dissociation constant (K(d)) of approximately 3 &mgr;M, whereas the affinity between Zn(2+) and the inactivated K(A) channels is 1000-fold lower. Zn(2+) therefore produces a concentration-dependent shift of the K(A) channel inactivation curve and enhances the K(A) current elicited from relatively positive holding potentials. It is also found that the kinetics of Zn(2+) action are fast enough to compete with the transition rates between different gating states of the channel. The rapid and selective binding of Zn(2+) to the closed K(A) channels keeps the channel in the closed state and explains the ion's concentration-dependent slowing effect on the activation of K(A) current. This in turn accounts for the inhibitory effect of Zn(2+) on the K(A) current elicited from hyperpolarized holding potentials. Because the molecular mechanisms underlying these gating changes are kinetic interactions between the binding-unbinding of Zn(2+) and the intrinsic gating processes of the channel, the shift of the inactivation curve and slowing of K(A) channel activation are quantitatively correlated with ambient Zn(2+) over a wide concentration range without "saturation"; i.e., The effects are already manifest in micromolar Zn(2+), yet are not saturated even in millimolar Zn(2+). Because the physiological concentration of Zn(2+) could vary over a similarly wide range according to neural activities, Zn(2+) may be a faithful physiological "fine tuner," controlling and controlled by neural activities through its effect on the K(A) current.