Properties of the inner pore region of TRPV1 channels revealed by block with quaternary ammoniums

The transient receptor potential vanilloid 1 (TRPV1) nonselective cationic channel is a polymodal receptor that activates in response to a wide variety of stimuli. To date, little structural information about this channel is available. Here, we used quaternary ammonium ions (QAs) of different sizes in an effort to gain some insight into the nature and dimensions of the pore of TRPV1. We found that all four QAs used, tetraethylammonium (TEA), tetrapropylammonium (TPrA), tetrabutylammonium, and tetrapentylammonium, block the TRPV1 channel from the intracellular face of the channel in a voltage-dependent manner, and that block by these molecules occurs with different kinetics, with the bigger molecules becoming slower blockers. We also found that TPrA and the larger QAs can only block the channel in the open state, and that they interfere with the channel's activation gate upon closing, which is observed as a slowing of tail current kinetics. TEA does not interfere with the activation gate, indicating that this molecule can reside in its blocking site even when the channel is closed. The dependence of the rate constants on the size of the blocker suggests a size of around 10 Å for the inner pore of TRPV1 channels.     

Selective disruption of high sensitivity heat activation but not capsaicin activation of TRPV1 channels by pore turret mutations

The capsaicin receptor transient receptor potential vanilloid (TRPV)1 is a highly heat-sensitive ion channel. Although chemical activation and heat activation of TRPV1 elicit similar pungent, painful sensation, the molecular mechanism underlying synergistic activation remains mysterious. In particular, where the temperature sensor is located and whether heat and capsaicin share a common activation pathway are debated. To address these fundamental issues, we searched for channel mutations that selectively affected one form of activation. We found that deletion of the first 10 amino acids of the pore turret significantly reduced the heat response amplitude and shifted the heat activation threshold, whereas capsaicin activation remained unchanged. Removing larger portions of the turret disrupted channel function. Introducing an artificial sequence to replace the deleted region restored sensitive capsaicin activation in these nonfunctional channels. The heat activation, however, remained significantly impaired, with the current exhibiting diminishing heat sensitivity to a level indistinguishable from that of a voltage-gated potassium channel, Kv7.4. Our results demonstrate that heat and capsaicin activation of TRPV1 are structurally and mechanistically distinct processes, and the pore turret is an indispensible channel structure involved in the heat activation process but is not part of the capsaicin activation pathway. Synergistic effect of heat and capsaicin on TRPV1 activation may originate from convergence of the two pathways on a common activation gate.     

Novel gating mechanism of polyamine block in the strong inward rectifier K channel Kir2.1

Inward rectifying K channels are essential for maintaining resting membrane potential and regulating excitability in many cell types. Previous studies have attributed the rectification properties of strong inward rectifiers such as Kir2.1 to voltage-dependent binding of intracellular polyamines or Mg to the pore (direct open channel block), thereby preventing outward passage of K ions. We have studied interactions between polyamines and the polyamine toxins philanthotoxin and argiotoxin on inward rectification in Kir2.1. We present evidence that high affinity polyamine block is not consistent with direct open channel block, but instead involves polyamines binding to another region of the channel (intrinsic gate) to form a blocking complex that occludes the pore. This interaction defines a novel mechanism of ion channel closure.     

Intrinsic versus extrinsic voltage sensitivity of blocker interaction with an ion channel pore

Many physiological and synthetic agents act by occluding the ion conduction pore of ion channels. A hallmark of charged blockers is that their apparent affinity for the pore usually varies with membrane voltage. Two models have been proposed to explain this voltage sensitivity. One model assumes that the charged blocker itself directly senses the transmembrane electric field, i.e., that blocker binding is intrinsically voltage dependent. In the alternative model, the blocker does not directly interact with the electric field; instead, blocker binding acquires voltage dependence solely through the concurrent movement of permeant ions across the field. This latter model may better explain voltage dependence of channel block by large organic compounds that are too bulky to fit into the narrow (usually ion-selective) part of the pore where the electric field is steep. To date, no systematic investigation has been performed to distinguish between these voltage-dependent mechanisms of channel block. The most fundamental characteristic of the extrinsic mechanism, i.e., that block can be rendered voltage independent, remains to be established and formally analyzed for the case of organic blockers. Here, we observe that the voltage dependence of block of a cyclic nucleotide–gated channel by a series of intracellular quaternary ammonium blockers, which are too bulky to traverse the narrow ion selectivity filter, gradually vanishes with extreme depolarization, a predicted feature of the extrinsic voltage dependence model. In contrast, the voltage dependence of block by an amine blocker, which has a smaller “diameter” and can therefore penetrate into the selectivity filter, follows a Boltzmann function, a predicted feature of the intrinsic voltage dependence model. Additionally, a blocker generates (at least) two blocked states, which, if related serially, may preclude meaningful application of a commonly used approach for investigating channel gating, namely, inferring the properties of the activation gate from the kinetics of channel block.     

State-dependent block of BK channels by synthesized shaker ball peptides

Crystal structures of potassium channels have strongly corroborated an earlier hypothetical picture based on functional studies, in which the channel gate was located on the cytoplasmic side of the pore. However, accessibility studies on several types of ligand-sensitive K(+) channels have suggested that their activation gates may be located near or within the selectivity filter instead. It remains to be determined to what extent the physical location of the gate is conserved across the large K(+) channel family. Direct evidence about the location of the gate in large conductance calcium-activated K(+) (BK) channels, which are gated by both voltage and ligand (calcium), has been scarce. Our earlier kinetic measurements of the block of BK channels by internal quaternary ammonium ions have raised the possibility that they may lack a cytoplasmic gate. We show in this study that a synthesized Shaker ball peptide (ShBP) homologue acts as a state-dependent blocker for BK channels when applied internally, suggesting a widening at the intracellular end of the channel pore upon gating. This is consistent with a gating-related conformational change at the cytoplasmic end of the pore-lining helices, as suggested by previous functional and structural studies on other K(+) channels. Furthermore, our results from two BK channel mutations demonstrate that similar types of interactions between ball peptides and channels are shared by BK and other K(+) channel types.     

Voltage-controlled gating at the intracellular entrance to a hyperpolarization-activated cation channel.

Hyperpolarization-activated cation (HCN) channels regulate pacemaking activity in cardiac cells and neurons. Our previous work using the specific HCN channel blocker ZD7288 provided evidence for an intracellular activation gate for these channels because it appears that ZD7288, applied from the intracellular side, can enter and leave HCN channels only at voltages where the activation gate is opened (Shin, K.S., B.S. Rothberg, and G. Yellen. 2001. J. Gen. Physiol. 117:91-101). However, the ZD7288 molecule is larger than the Na(+) or K(+) ions that flow through the open channel. In the present study, we sought to resolve whether the voltage gate at the intracellular entrance to the pore for ZD7288 also can be a gate for permeant ions in HCN channels. Single residues in the putative pore-lining S6 region of an HCN channel (cloned from sea urchin; spHCN) were substituted with cysteines, and the mutants were probed with Cd(2+) applied to the intracellular side of the channel. One mutant, T464C, displayed rapid irreversible block when Cd(2+) was applied to opened channels, with an apparent blocking rate of approximately 3 x 10(5) M(-1)s(-1). The blocking rate was decreased for channels held at more depolarized voltages that close the channels, which is consistent with the Cd(2+) access to this residue being gated from the intracellular side of the channel. 464C channels could be recovered from Cd(2+) inhibition in the presence of a dithiol applied to the intracellular side. The rate of this recovery also was reduced when channels were held at depolarized voltages. Finally, Cd(2+) could be trapped inside channels that were composed of WT/464C tandem-linked subunits, which could otherwise recover spontaneously from Cd(2+) inhibition. Thus, Cd(2+) escape is also gated at the intracellular side of the channel. Together, these results are consistent with a voltage-controlled structure at the intracellular side of the spHCN channel that can gate the flow of cations through the pore.     

Y3+ block demonstrates an intracellular activation gate for the alpha1G T-type Ca2+ channel

Classical electrophysiology and contemporary crystallography suggest that the activation gate of voltage-dependent channels is on the intracellular side, but a more extracellular "pore gate" has also been proposed. We have used the voltage dependence of block by extracellular Y(3+) as a tool to locate the activation gate of the alpha1G (Ca(V)3.1) T-type calcium channel. Y(3+) block exhibited no clear voltage dependence from -40 to +40 mV (50% block at 25 nM), but block was relieved rapidly by stronger depolarization. Reblock of the open channel, reflected in accelerated tail currents, was fast and concentration dependent. Closed channels were also blocked by Y(3+) at a concentration-dependent rate, only eightfold slower than open-channel block. When extracellular Ca(2+) was replaced with Ba(2+), the rate of open block by Y(3+) was unaffected, but closed block was threefold faster than in Ca(2+), suggesting the slower closed-block rate reflects ion-ion interactions in the pore rather than an extracellularly located gate. Since an extracellular blocker can rapidly enter the closed pore, the primary activation gate must be on the intracellular side of the selectivity filter.     

The pore helix dipole has a minor role in inward rectifier channel function

Ion channels lower the energetic barrier for ion passage across cell membranes and enable the generation of bioelectricity. Electrostatic interactions between permeant ions and channel pore helix dipoles have been proposed as a general mechanism for facilitating ion passage. Here, using genetic selections to probe interactions of an exemplar potassium channel blocker, barium, with the inward rectifier Kir2.1, we identify mutants bearing positively charged residues in the potassium channel signature sequence at the pore helix C terminus. We show that these channels are functional, selective, resistant to barium block, and have minimally altered conductance properties. Both the experimental data and model calculations indicate that barium resistance originates from electrostatics. We demonstrate that potassium channel function is remarkably unperturbed when positive charges occur near the permeant ions at a location that should counteract pore helix electrostatic effects. Thus, contrary to accepted models, the pore helix dipole seems to be a minor factor in potassium channel permeation.     

Blocker state dependence and trapping in hyperpolarization-activated cation channels: evidence for an intracellular activation gate

Hyperpolarization-activated cation currents (I(h)) are key determinants of repetitive electrical activity in heart and nerve cells. The bradycardic agent ZD7288 is a selective blocker of these currents. We studied the mechanism for ZD7288 blockade of cloned I(h) channels in excised inside-out patches. ZD7288 blockade of the mammalian mHCN1 channel appeared to require opening of the channel, but strong hyperpolarization disfavored blockade. The steepness of this voltage-dependent effect (an apparent valence of approximately 4) makes it unlikely to arise solely from a direct effect of voltage on blocker binding. Instead, it probably indicates a differential affinity of the blocker for different channel conformations. Similar properties were seen for ZD7288 blockade of the sea urchin homologue of I(h) channels (SPIH), but some of the blockade was irreversible. To explore the molecular basis for the difference in reversibility, we constructed chimeric channels from mHCN1 and SPIH and localized the structural determinant for the reversibility to three residues in the S6 region likely to line the pore. Using a triple point mutant in S6, we also revealed the trapping of ZD7288 by the closing of the channel. Overall, the observations led us to hypothesize that the residues responsible for ZD7288 block of I(h) channels are located in the pore lining, and are guarded by an intracellular activation gate of the channel.     

Block of the cyclic GMP-gated channel of vertebrate rod and cone photoreceptors by l-cis-diltiazem.

Inside-out patches were excised from catfish rod or cone outer segments. Single channel and macroscopic currents were recorded from GMP-gated channels activated by 1 mM cGMP in low divalent buffered saline. Currents were blocked by the application of micromolar concentrations of l-cis-diltiazem to the cytoplasmic side of the patch. The concentration dependence of block indicated that a single molecule was sufficient to block a channel and that all channels were susceptible to block. The dissociation constant for the rod channel was an order of magnitude smaller than for the cone channel, but the voltage dependence of block was nearly identical. The macroscopic current-voltage relation in the presence of blocker was inwardly rectifying and superficially resembled voltage-dependent block by an impermeant blocker occluding the ion-conducting pore of the channel. Block by diltiazem acting from the extracellular side of the channel was investigated by including 5 microM diltiazem in the recording pipette solution. The macroscopic current-voltage relation again showed inward rectification, inconsistent with the idea that diltiazem acts by occluding the pore at the external side. The kinetics of block by diltiazem applied to the intra- and extracellular side were measured in cone patches containing only a single channel. The unbinding rates were similar in both cases, suggesting a single binding site. Differences in the binding rate were consistent with greater accessibility to the binding site from the cytoplasmic side. Block from the cytoplasmic side was independent of pH, suggesting that the state of ionization of diltiazem was not related to its ability to block the channel in a voltage-dependent fashion. These observations are inconsistent with a pore-occluding blocker, but could be explained if the hydrophobic portion of diltiazem partitioned into the hydrophobic core of the channel protein, perhaps altering the gating of the channel.     

The inner quaternary ammonium ion receptor in potassium channels of the node of Ranvier

Quaternary ammonium ions were applied to the inside of single myelinated nerve fibers by diffusion from a cut end. The resulting block of potassium channels in the node of Ranvier was studied under voltage-clamp conditions. The results agree in almost all respects with similar studies by Armstrong of squid giant axons. With tetraethylammonium ion (TEA), pentyltriethylammonium ion (C₅), or nonyltriethylammonium ion (C₉) inside the node, potassium current during a depolarization begins to rise at the normal rate, reaches a peak, and then falls again. This unusual inactivation is more complete with C₉ than with TEA. Larger depolarizations give more block. Thus the block of potassium channels grows with time and voltage during a depolarization. The block reverses with repolarization, but for C₉ full reversal takes seconds at -75 mv. The reversal is faster in 120 mM KCl Ringer''s and slower during a hyperpolarization to -125 mv. All of these effects contrast with the time and voltage-independent block of potassium, channels seen with external quaternary ammonium ions on the node of Ranvier. External TEA, C₅, and C₉ block without inactivation. The external quaternary ammonium ion receptor appears to be distinct from the inner one. Apparently the inner quaternary ammonium ion receptor can be reached only when the activation gate for potassium channels is open. We suggest that the inner receptor lies within the channel and that the channel is a pore with its activation gate near the axoplasmic end.     

Gating of acid-sensitive ion channel-1: release of Ca2+ block vs. allosteric mechanism

The acid-sensitive ion channels (ASICs) are a family of voltage-insensitive sodium channels activated by external protons. A previous study proposed that the mechanism underlying activation of ASIC consists of the removal of a Ca2+ ion from the channel pore (Immke and McCleskey, 2003). In this work we have revisited this issue by examining single channel recordings of ASIC1 from toadfish (fASIC1). We demonstrate that increases in the concentration of external protons or decreases in the concentration of external Ca2+ activate fASIC1 by progressively opening more channels and by increasing the rate of channel opening. Both maneuvers produced similar effects in channel kinetics, consistent with the former notion that protons displace a Ca2+ ion from a high-affinity binding site. However, we did not observe any of the predictions expected from the release of an open-channel blocker: decrease in the amplitude of the unitary currents, shortening of the mean open time, or a constant delay for the first opening when the concentration of external Ca2+ was decreased. Together, the results favor changes in allosteric conformations rather than unblocking of the pore as the mechanism gating fASIC1. At high concentrations, Ca2+ has an additional effect that consists of voltage-dependent decrease in the amplitude of unitary currents (EC50 of 10 mM at -60 mV and pH 6.0). This phenomenon is consistent with voltage-dependent block of the pore but it occurs at concentrations much higher than those required for gating.     

An inhibitor of TRPV1 channels isolated from funnel Web spider venom

Capsaicin receptor channels (TRPV1) are nonselective cation channels that integrate multiple noxious stimuli in sensory neurons. In an effort to identify new inhibitors of these channels we screened a venom library for activity against TRPV1 channels and found robust inhibitory activity in venom from Agelenopsis aperta, a north American funnel web spider. Fractionation of the venom using reversed-phase HPLC resulted in the purification of two acylpolyamine toxins, AG489 and AG505, which inhibit TRPV1 channels from the extracellular side of the membrane. The activity of AG489 was characterized further, and the toxin was found to inhibit TRPV1 channels with a K(i) of 0.3 microM at -40 mV. Inhibition of TRPV1 channels by AG489 is strongly voltage-dependent, with relief of inhibition at positive voltages, consistent with the toxin inhibiting the channel through a pore-blocking mechanism. We used scanning mutagenesis throughout the TM5-TM6 linker, a region thought to form the outer pore of TRPV1 channels, to identify pore mutations that alter toxin affinity. Four mutants dramatically decrease toxin affinity and several mutants increase toxin affinity, consistent with the notion that the TM5-TM6 linker forms the outer vestibule of TRPV1 channels and that AG489 is a pore blocker.     

Biphasic currents evoked by chemical or thermal activation of the heat-gated ion channel, TRPV3

2-Aminoethyl diphenylborinate was recently identified as a chemical activator of TRPV1, TRPV2, and TRPV3, three heat-gated members of the transient receptor potential vanilloid (TRPV) ion channel subfamily. Here we demonstrated that two structurally related compounds, diphenylboronic anhydride (DPBA) and diphenyltetrahydrofuran (DPTHF), can also modulate the activity of these channels. DPBA acted as a TRPV3 agonist, whereas DPTHF exhibited prominent antagonistic activity. However, all three diphenyl-containing compounds promoted some degree of channel activation or potentiation, followed by channel block. Strong TRPV3 activation by DPBA often leads to the appearance of a secondary, enhanced, current phase. A similar biphasic response was observed during TRPV3 heat stimulation; an initial, gradually sensitizing phase (I(1)) was followed by an abrupt transition to a secondary phase (I(2)). I(2) was characterized by larger current amplitude, loss of outward rectification, and alterations in the following properties: permeability among cations; ruthenium red and DPTHF sensitivity; temperature dependence; and voltage-dependent gating. The I(1) to I(2) transition depended strongly on TRPV3 current density. Removal of extracellular divalent cations resulted in heat-evoked currents resembling I(2), whereas mutation of a putative Ca(2+)-binding residue in the pore loop domain, aspartate 641, facilitated detection of the I(1) to I(2) transition, suggesting that the conversion to I(2) resulted from the agonist- and time-dependent loss of divalent cationic inhibition. Primary keratinocytes overexpressing exogenous TRPV3 also exhibited biphasic agonist-evoked currents. Thus, strong activation by either chemical or thermal stimuli led to biphasic TRPV3 signaling behavior that may be associated with changes in the channel pore.     

Ionic permeation and conduction properties of neuronal KCNQ2/KCNQ3 potassium channels

Heteromeric KCNQ2/3 potassium channels are thought to underlie the M-current, a subthreshold potassium current involved in the regulation of neuronal excitability. KCNQ channel subunits are structurally unique, but it is unknown whether these structural differences result in unique conduction properties. Heterologously expressed KCNQ2/3 channels showed a permeation sequence of while showing a conduction sequence of A differential contribution of component subunits to the properties of heteromeric KCNQ2/3 channels was demonstrated by studying homomeric KCNQ2 and KCNQ3 channels, which displayed contrasting ionic selectivities. KCNQ2/3 channels did not exhibit an anomalous mole-fraction effect in mixtures of K(+) and Rb(+). However, extreme voltage-dependence of block by external Cs(+) was indicative of multi-ion pore behavior. Block of KCNQ2/3 channels by external Ba(2+) ions was voltage-independent, demonstrating unusual ionic occupation of the outer pore. Selectivity properties and block of KCNQ2 were altered by mutation of outer pore residues in a manner consistent with the presence of multiple ion-binding sites. KCNQ2/3 channel deactivation kinetics were slowed exclusively by Rb(+), whereas activation of KCNQ2/3 channels was altered by a variety of external permeant ions. These data indicate that KCNQ2/3 channels are multi-ion pores which exhibit distinctive mechanisms of ion conduction and gating.     

Mechanism of intracellular block of the KcsA K+ channel by tetrabutylammonium: insights from X-ray crystallography, electrophysiology and replica-exchange molecular dynamics simulations

The mechanism of intracellular blockade of the KcsA potassium channel by tetrabutylammonium (TBA) is investigated through functional, structural and computational studies. Using planar-membrane electrophysiological recordings, we characterize the binding kinetics as well as the dependence on the transmembrane voltage and the concentration of the blocker. It is found that the apparent affinity of the complex is significantly greater than that of any of the eukaryotic K(+) channels studied previously, and that the off-rate increases with the applied transmembrane voltage. In addition, we report a crystal structure of the KcsA-TBA complex at 2.9 A resolution, with TBA bound inside the large hydrophobic cavity located at the center of the channel, consistent with the results of previous functional and structural studies. Of particular interest is the observation that the presence of TBA has a negligible effect on the channel structure and on the position of the potassium ions occupying the selectivity filter. Inspection of the electron density corresponding to TBA suggests that the ligand may adopt more than one conformation in the complex, though the moderate resolution of the data precludes a definitive interpretation on the basis of the crystallographic refinement methods alone. To provide a rationale for these observations, we carry out an extensive conformational sampling of an atomic model of TBA bound in the central cavity of KcsA, using the Hamiltonian replica-exchange molecular dynamics simulation method. Comparison of the simulated and experimental density maps indicates that the latter does reflect at least two distinct binding orientations of TBA. The simulations show also that the relative population of these binding modes is dependent on the ion configuration occupying the selectivity filter, thus providing a clue to the nature of the voltage-dependence of the binding kinetics.     

Selectivity filter gating in large-conductance Ca(2+)-activated K+ channels

Membrane voltage controls the passage of ions through voltage-gated K (K(v)) channels, and many studies have demonstrated that this is accomplished by a physical gate located at the cytoplasmic end of the pore. Critical to this determination were the findings that quaternary ammonium ions and certain peptides have access to their internal pore-blocking sites only when the channel gates are open, and that large blocking ions interfere with channel closing. Although an intracellular location for the physical gate of K(v) channels is well established, it is not clear if such a cytoplasmic gate exists in all K(+) channels. Some studies on large-conductance, voltage- and Ca(2+)-activated K(+) (BK) channels suggest a cytoplasmic location for the gate, but other findings question this conclusion and, instead, support the concept that BK channels are gated by the pore selectivity filter. If the BK channel is gated by the selectivity filter, the interactions between the blocking ions and channel gating should be influenced by the permeant ion. Thus, we tested tetrabutyl ammonium (TBA) and the Shaker "ball" peptide (BP) on BK channels with either K(+) or Rb(+) as the permeant ion. When tested in K(+) solutions, both TBA and the BP acted as open-channel blockers of BK channels, and the BP interfered with channel closing. In contrast, when Rb(+) replaced K(+) as the permeant ion, TBA and the BP blocked both closed and open BK channels, and the BP no longer interfered with channel closing. We also tested the cytoplasmically gated Shaker K channels and found the opposite behavior: the interactions of TBA and the BP with these K(v) channels were independent of the permeant ion. Our results add significantly to the evidence against a cytoplasmic gate in BK channels and represent a positive test for selectivity filter gating.     

The pore structure and gating mechanism of K2P channels

Two-pore domain (K2P) potassium channels are important regulators of cellular electrical excitability. However, the structure of these channels and their gating mechanism, in particular the role of the bundle-crossing gate, are not well understood. Here, we report that quaternary ammonium (QA) ions bind with high-affinity deep within the pore of TREK-1 and have free access to their binding site before channel activation by intracellular pH or pressure. This demonstrates that, unlike most other K(+) channels, the bundle-crossing gate in this K2P channel is constitutively open. Furthermore, we used QA ions to probe the pore structure of TREK-1 by systematic scanning mutagenesis and comparison of these results with different possible structural models. This revealed that the TREK-1 pore most closely resembles the open-state structure of KvAP. We also found that mutations close to the selectivity filter and the nature of the permeant ion profoundly influence TREK-1 channel gating. These results demonstrate that the primary activation mechanisms in TREK-1 reside close to, or within the selectivity filter and do not involve gating at the cytoplasmic bundle crossing.     

Outer pore architecture of a Ca2+-selective TRP channel

The TRP superfamily forms a functionally important class of cation channels related to the product of the Drosophila trp gene. TRP channels display an unusual diversity in activation mechanisms and permeation properties, but the basis of this diversity is unknown, as the structure of these channels has not been studied in detail. To obtain insight in the pore architecture of TRPV6, a Ca(2+)-selective member of the TRPV subfamily, we probed the dimensions of its pore and determined pore-lining segments using cysteine-scanning mutagenesis. Based on the permeability of the channel to organic cations, we estimated a pore diameter of 5.4 A. Mutating Asp(541), a residue involved in high affinity Ca(2+) binding, altered the apparent pore diameter, indicating that this residue lines the narrowest part of the pore. Cysteines introduced in a region preceding Asp(541) displayed a cyclic pattern of reactivity to Ag(+) and cationic methylthio-sulfanate reagents, indicative of a pore helix. The anionic methanethiosulfonate ethylsulfonate showed only limited reactivity in this region, consistent with the presence of a cation-selective filter at the outer part of the pore helix. Based on these data and on homology with the bacterial KcsA channel, we present the first structural model of a TRP channel pore. We conclude that main structural features of the outer pore, namely a selectivity filter preceded by a pore helix, are conserved between K(+) channels and TRPV6. However, the selectivity filter of TRPV6 is wider than that of K(+) channels and lined by amino acid side chains rather than main chain carbonyls.     

Internal block of human heart sodium channels by symmetrical tetra- alkylammoniums

The human heart Na channel (hH1) was expressed by transient transfection in tsA201 cells, and we examined the block of Na current by a series of symmetrical tetra-alkylammonium cations: tetramethylammonium (TMA), tetraethylammonium (TEA), tetrapropylammonium (TPrA), tetrabutylammonium (TBA), and tetrapentylammonium (TPeA). Internal TEA and TBA reduce single-channel current amplitudes while having little effect on single channel open times. The reduction in current amplitude is greater at more depolarized membrane potentials. Analysis of the voltage-dependence of single-channel current block indicates that TEA, TPrA and TBA traverse a fraction of 0.39, 0.52, and 0.46 of the membrane electric field to reach their binding sites. Rank potency determined from single-channel experiments indicates that block increases with the lengths of the alkyl side chains (TBA > TPrA > TEA > TMA). Internal TMA, TEA, TPrA, and TBA also reduce whole-cell Na currents in a voltage-dependent fashion with increasing block at more depolarized voltages, consistent with each compound binding to a site at a fractional distance of 0.43 within the membrane electric field. The correspondence between the voltage dependence of the block of single-channel and macroscopic currents indicates that the blockers do not distinguish open from closed channels. In support of this idea TPrA has no effect on deactivation kinetics, and therefore does not interfere with the closing of the activation gates. At concentrations that substantially reduce Na channel currents, TMA, TEA, and TPrA do not alter the rate of macroscopic current inactivation over a wide range of voltages (-50 to +80 mV). Our data suggest that TMA, TEA, and TPrA bind to a common site deep within the pore and block ion transport by a fast-block mechanism without affecting either activation or inactivation. By contrast, internal TBA and TPeA increase the apparent rate of inactivation of macroscopic currents, suggestive of a block with slower kinetics.