Kir5.1 underlies long-lived subconductance levels in heteromeric Kir4.1/Kir5.1 channels from Xenopus tropicalis

The inwardly-rectifying potassium channel subunit Kir5.1 selectively co-assembles with members of the Kir4.0 subfamily to form novel pH-sensitive heteromeric channels with unique single channel properties. In this study, we have cloned orthologs of Kir4.1 and Kir5.1 from the genome of the amphibian, Xenopus tropicalis (Xt). Heteromeric XtKir4.1/XtKir5.1 channels exhibit similar macroscopic current properties to rat Kir4.1/Kir5.1 with a faster time-dependent rate of activation. However, single channel analysis of heteromeric XtKir4.1/XtKir5.1 channels reveals that they have markedly different long-lived, multi-level subconductance states. Furthermore, we demonstrate that the XtKir5.1 subunit is responsible for these prominent subconductance levels. These results are consistent with a model in which the slow transitions between sublevel states represent the movement of individual subunits. These novel channels now provide an excellent model system to determine the structural basis of subconductance levels and contribution of heteromeric pore architecture to this process.     

Hidden Markov model analysis of intermediate gating steps associated with the pore gate of shaker potassium channels.

Cooperativity among the four subunits helps give rise to the remarkable voltage sensitivity of Shaker potassium channels, whose open probability changes tenfold for a 5-mV change in membrane potential. The cooperativity in these channels is thought to arise from a concerted structural transition as the final step in opening the channel. Recordings of single-channel ionic currents from certain other channel types, as well as our previous recordings from T442S mutant Shaker channels, however, display intermediate conductance levels in addition to the fully open and closed states. These sublevels might represent stepwise, rather than concerted, transitions in the final steps of channel activation. Here, we report a similar fine structure in the closing transitions of Shaker channels lacking the mutation. Describing the deactivation time course with hidden Markov models, we find that two subconductance levels are rapidly traversed during most closing transitions of chimeric, high conductance Shaker channels. The lifetimes of these levels are voltage-dependent, with maximal values of 52 and 22 micros at -100 mV, and the voltage dependences of transitions among these states suggest that they arise from equivalent conformational changes occurring in individual subunits. At least one subconductance level is found to be traversed in normal conductance Shaker channels. We speculate that voltage-dependent conformational changes in the subunits give rise to changes in a "pore gate" associated with the selectivity filter region of the channel, producing the subconductance states. As a control for the hidden Markov analysis, we applied the same procedures to recordings of the recovery from N-type inactivation in Shaker channels. These transitions are found to be instantaneous in comparison.     

Intermediate Conductances during Deactivation of Heteromultimeric Shaker Potassium Channels

A previous study of the T442S mutant Shaker channel revealed activation-coupled subconductance levels that apparently represent kinetic intermediates in channel activation (Zheng, J., and F.J. Sigworth. 1997. J. Gen. Physiol. 110:101–117). We have now extended the study to heteromultimeric channels consisting of various numbers of mutant subunits as well as channels without mutant subunits, all in the background of a chimeric Shaker channel having increased conductance. It has been found that activation-coupled sublevels exist in all these channel types, and are traversed in at least 80% of all deactivation time courses. In symmetric K⁺ solutions, the currents in the two sublevels have a linear voltage dependence, being 23–44% and 54–70% of the fully open conductance. Sublevels in different channel types share similar voltage dependence of the mean lifetime and similar ion selectivity properties. However, the mean lifetime of each current level depends approximately geometrically on the number of mutant subunits in the channel, becoming shorter in channels having fewer mutant subunits. Each mutant subunit appears to stabilize all of the conducting states by ∼0.5 kcal/mol. Consistent with previous results in the mutant channel, sublevels in channels with two or no mutant subunits also showed ion selectivities that differ from that of the fully open level, having relatively higher K⁺ than Rb⁺ conductances. A model is presented in which Shaker channels have two coupled activation gates, one associated with the selectivity filter and a second associated with the S6 helix bundle.     

Independent gating of single pores in CLC-0 chloride channels.

The Cl- channel from the Torpedo electric organ, CLC-0, is the prototype of a large gene family of Cl- channels. At the single-channel level, CLC-0 shows a "double-barreled" behavior. Recently it was shown that CLC-0 is a dimer, and it was suggested that each subunit forms a single pore. The two protopores are gated individually by a fast voltage and anion-dependent gating mechanism. A slower common gating mechanism operates on both pores simultaneously. Previously, wild-type/mutant heteromeric channels had been constructed that display a large wild-type pore and small mutant pore. Here we use patch-clamp recording of single wild-type and mutant CLC-0 channels to investigate in detail the dependence of the gating of one protopore on the physically attached neighboring pore. No difference in rate constants of opening and closing of protopores could be found comparing homomeric wild-type and heteromeric wild-type/mutant channels. In addition, detailed kinetic analysis reveals that gating of single subunits is not correlated with the gating of the neighboring subunit. The results are consistent with the view that permeation and fast gating of individual pores are fully independent of the neighboring pore. Because the two subunits are associated in a common protein complex, opening and closing transitions of individual pores are probably due to only small conformational changes in each pore. In addition to the fast and slow gating mechanisms known previously for CLC-0, in the course of this study we occasionally observed an additional gating process that led to relatively long closures of single pores.     

Gating of heteromeric retinal rod channels by cyclic AMP: role of the C-terminal and pore domains

Cyclic nucleotide-gated channels are tetramers composed of homologous alpha and beta subunits. C-terminal truncation mutants of the alpha and beta subunits of the retinal rod channel were expressed in Xenopus oocytes, and analyzed for cGMP- and cAMP-induced currents (single-channel records and macroscopic currents). When the alpha subunit truncated downstream of the cGMP-binding site (alpha D608stop) is co-injected with truncated beta subunits, the heteromeric channels present a drastic increase of cAMP sensitivity. A partial effect is observed with heteromeric alpha R656stop-containing channels, while alpha K665stop-containing channels behave like alpha wt/beta wt. The three truncated alpha subunits have wild-type activity when expressed alone. Heteromeric channels composed of alpha wt or truncated alpha subunits and chimeric beta subunits containing the pore domain of the alpha subunit have the same cAMP sensitivity as alpha-only channels. The results disclose the key role of two domains distinct from the nucleotide binding site in the gating of heteromeric channels by cAMP: the pore of the beta subunit, which has an activating effect, and a conserved domain situated downstream of the cGMP-binding site in the alpha subunit (I609-K665), which inhibits this effect.     

Heteromeric AMPA receptors assemble with a preferred subunit stoichiometry and spatial arrangement.

AMPA receptors are thought to be a tetrameric assembly of the subunits GluR1-4. We have examined whether two coexpressed subunits (GluR1/2) combine at random to form channels, or preferentially assemble with a specific stoichiometry and spatial configuration. The subunits carried markers controlling ion permeation and desensitization, and these properties were monitored as a function of relative expression level and subunit composition. Homomeric receptors assembled stochastically while heteromeric receptors preferentially formed with a stoichiometry of two GluR1 and two GluR2 subunits, and with identical subunits positioned on opposite sides of the channel pore. This structure will predominate if GluR1 binds to GluR2 more rapidly during receptor assembly than other subunit combinations. The practical outcome of selective heteromeric assembly is a more homogenous receptor population in vivo.     

Mutations in the putative pore-forming segment favor short-lived wild-type Kir2.1 pore conformations

We have characterized single and double mutations in the M1-M2 segment of an inwardly rectifying K(+) channel, Kir2.1, using the cell-attached configuration of the patch-clamp technique. These mutations generated novel N-glycosylation sites at positions 128, 140, 143, and 147. Previously, we showed that these mutants were glycosylated, functional, and at the cell surface, which indicated that the putative pore-forming segment, including the invariant G(Y/F)G sequence of K(+) channels, was extracellular [Schwalbe, R. A., Rudin, A., Xia, S.-L., and Wingo, C. S. (2002) J. Biol. Chem. 277, 24382-24389]. In this study, three conductance states, corresponding to the main open state and two subconductance states, were identified in WT Kir2.1 channels expressed in infected Sf9 cells. Kir2.1 channels with mutations in the M1-M2 linker had at least one distinguishable conductance state of WT channels. In addition, these mutations altered the transitions, duration, and frequency of the defined populations of permeating and nonpermeating states. Of note, S128N had permeation rates similar to those of WT Kir2.1, but the total duration of the lower subconductance state was 3-5 times longer. Mutations in the signature sequence, I143N/Y145T, produced channels with permeation rates similar to those of the main open state and lower subconductance state of WT Kir2.1; however, the frequencies of these states were substantially different. These results demonstrate a novel functional role of the M1-M2 segment in regulating the transitions of the Kir2.1 channel and therefore suggest that this segment is a critical structural determinant in adjustments of pore conformations. Additionally, our results indicate that these mutants are correctly folded and thus further substantiate that the M1-M2 segment, including the G(Y/F)G sequence, is topologically extracellular.     

Achromatopsia-associated mutation in the human cone photoreceptor cyclic nucleotide-gated channel CNGB3 subunit alters the ligand sensitivity and pore properties of heteromeric channels

Cone photoreceptor cyclic nucleotide-gated (CNG) channels are thought to form by assembly of two different subunit types, CNGA3 and CNGB3. Recently, mutations in the gene encoding the CNGB3 subunit have been linked to achromatopsia in humans. Here we describe the functional consequences of two achromatopsia-associated mutations in human CNGB3 (hCNGB3). Co-expression in Xenopus oocytes of human CNGA3 (hCNGA3) subunits with hCNGB3 subunits containing an achromatopsia-associated mutation in the S6 transmembrane domain (S435F) generated functional heteromeric channels that exhibited an increase in apparent affinity for both cAMP and cGMP compared with wild type heteromeric channels. In contrast, co-expression of a presumptive null mutation of hCNGB3 (T383f.s.Delta C) with hCNGA3 produced channels with properties indistinguishable from homomeric hCNGA3 channels. The effect of hCNGB3 S435F subunits on cell-surface expression of green fluorescent protein-tagged hCNGA3 subunits and of non-tagged hCNGA3 subunits on surface expression of green fluorescent protein-hCNGB3 S435F subunits were similar to those observed for wild type hCNGB3 subunits, suggesting that the mutation does not grossly disturb subunit assembly or plasma membrane targeting. The S435F mutation was also found to produce changes in the pore properties of the channel, including decreased single channel conductance and decreased sensitivity to block by l-cis-diltiazem. Overall, these results suggest that the functional properties of cone CNG channels may be altered in patients with the S435F mutation, providing evidence supporting the pathogenicity of this mutation in humans. Thus, achromatopsia may arise from a disturbance of cone CNG channel gating and permeation or from the absence of functional CNGB3 subunits.     

Single-channel properties of ionic channels gated by cyclic nucleotides.

This paper presents an extensive analysis of single-channel properties of cyclic nucleotide gated (CNG) channels, obtained by injecting into Xenopus laevis oocytes the mRNA encoding for the alpha and beta subunits from bovine rods. When the alpha and beta subunits of the CNG channel are coexpressed, at least three types of channels with different properties are observed. One type of channel has well-resolved, multiple conductive levels at negative voltages, but not at positive voltages. The other two types of channel are characterized by flickering openings, but are distinguished because they have a low and a high conductance. The alpha subunit of CNG channels has a well-defined conductance of about 28 pS, but multiple conductive levels are observed in mutant channels E363D and T364M. The conductance of these open states is modulated by protons and the membrane voltage, and has an activation energy around 44 kJ/mol. The relative probability of occupying any of these open states is independent of the cGMP concentration, but depends on extracellular protons. The open probability in the presence of saturating cGMP was 0.78, 0.47, 0.5, and 0.007 in the w.t. and mutants E363D, T364M, and E363G, and its dependence on temperature indicates that the thermodynamics of the transition between the closed and open state is also affected by mutations in the pore region. These results suggest that CNG channels have different conductive levels, leading to the existence of multiple open states in homomeric channels and to the flickering behavior in heteromeric channels, and that the pore is an essential part of the gating of CNG channels.     

Two different conformational states of the KirBac3.1 potassium channel revealed by electron crystallography

Potassium channels allow the selective flow of K(+) ions across membranes. In response to external gating signals, the potassium channel can move reversibly through a series of structural conformations from a closed to an open state. 2D crystals of the inwardly rectifying K(+) channel KirBac3.1 from Magnetospirillum magnetotacticum have been captured in two distinct conformations, providing "snap shots" of the gating process. Analysis by electron cryomicroscopy of these KirBac3.1 crystals has resulted in reconstructed images in projection at 9 A resolution. Kir channels are tetramers of four subunits arranged as dimers of dimers. Each subunit has two transmembrane helices (inner and outer). In one crystal form, the pore is blocked; in the other crystal form, the pore appears open. Modeling based on the KirBac1.1 (closed) crystal structure shows that opening of the ion conduction pathway could be achieved by bending of the inner helices and significant movements of the outer helices.     

Cytoplasmic acidosis induces multiple conductance states in ATP-sensitive potassium channels of cardiac myocytes

We studied the effect of cytoplasmic acidosis on the ionic conducting states of ATP-sensitive potassium channels in heart ventricular cells of guinea pigs and rabbits by using a patch-clamp technique with inside-out patch configuration. Under normal conditions (pH 7.4), the channel alternated between a closed state and a main open state in the absence of nucleotides on the cytoplasmic side. As internal pH was reduced below 6.5, the single channel current manifested distinct subconductance levels. The probability of the appearance of these subconductance levels was pH dependent with a greater probability of subconductance states at lower pH. A variance-mean amplitude analysis technique revealed two subconductance levels approximately equally spaced between the main open level and the closed level (63 and 33%). A current-voltage plot of the two subconductance levels and the main level showed that they had similar reversal potentials and rectification properties. An intrinsic flickering gating property characteristic of these ATP-sensitive channels was found unchanged in the 63% subconductance state, suggesting that this subconductance state and the main conductance state share similar ion pore properties (including ion selection and block) and similar gating mechanisms. The appearance of the subconductance states decreased as ionic strength was increased, and the subconductance states were also slightly voltage dependent, suggesting an electrostatic interaction between the protons and the negative surface charge in the vicinity of the binding sites, which may be close to the inner entrance of the ion pore. Proteolytic modification of the channel on the cytoplasmic side with trypsin did not abolish the subconductance levels. External acidosis did not induce subconductance levels. These results suggest that protons bound to the negatively charged group at the inner entrance of the channel ion pore may induce conformational changes, leading to partially reduced conductance states.     

Subconductance States of a Mutant NMDA Receptor Channel Kinetics,Calcium, and Voltage Dependence

The kinetic properties of main and subconductance states of a mutant mouse N-methyl-d-aspartate (NMDA) receptor channel were examined. Recombinant receptors made of ζ-ε₂ (NR1-NR2B) subunits having asparagine-to-glutamine mutations in the M2 segment (ζN598Q /ε₂N589Q) were expressed in Xenopus oocytes. Single channel currents recorded from outside-out patches were analyzed using hidden Markov model techniques. In Ca²⁺-free solutions, an open receptor channel occupies a main conductance (93 pS) and a subconductance (62 pS) with about equal probability. There are both brief and long-lived subconductance states, but only a single main level state. At −80 mV, the lifetime of the main and the longer-lived sub level are both ∼3.3 ms. The gating of the pore and the transition between conductance levels are essentially independent processes. Surprisingly, hyperpolarization speeds both the sub-to-main and main-to-sub transition rate constants (∼120 mV/e-fold change), but does not alter the equilibrium occupancies. Extracellular Ca²⁺ does not influence the transition rate constants. We conclude that the subconductance levels arise from fluctuations in the energetics of ion permeation through a single pore, and that the voltage dependence of these fluctuations reflects the modulation by the membrane potential of the barrier between the main and subconductance conformations of the pore.     

Peptide backbone chemistry and membrane channel function: effects of a single amide-to-ester replacement on gramicidin channel structure and function

To examine the structural and functional importance of backbone amide groups in ion channels for subunit folding, hydrogen bonding, ion solvation, and ion permeation, we replaced the peptide bond between Val(1) and Gly(2) in gramicidin A by an ester bond. The substitution is at the junction between the two channel subunits, where it removes an intramolecular hydrogen bond between the NH of Gly(2) and the C==O of Val(7) and perturbs an intermolecular hydrogen bond between the C==O of Val(1) in one subunit and the NH of Ala(5) in the other subunit. The substitution thus perturbs not only subunit folding but also dimer assembly, in addition to any effects on ion permeation. This backbone modification has large effects on channel function: It alters channel stability, as monitored by the channel forming ability and channel lifetime, and ion permeability, as monitored by changes in single-channel conductance and cation permeability ratios. In fact, the homodimeric channels, with two ester-containing subunits, have lifetimes so short that it becomes impossible to characterize them in any detail. The peptide --> ester substitution, however, does not affect the basic subunit fold because heterodimeric channels can form between a subunit with an ester bond and a native subunit. These heterodimeric channels, with only a single ester bond, are more easily characterized; the lone ester reduces the single-channel conductance about 4-fold and the lifetime about 200-fold as compared to the native homodimeric channels. The altered channel function results from a perturbation/disruption of the hydrogen bond network that stabilizes the backbone, as well as the membrane-spanning dimer, and that forms the lining of the ion-conducting pore. Molecular dynamics simulations show the expected destabilization of the modified heterodimeric or homodimeric channels, but the changes in backbone structure and dynamics are remarkably small. The ester bond is somewhat unstable, which precluded further structural characterization. The lability also led to a hydrolysis product that terminates with an alcohol and lacks formyl-Val. Symmetric channels formed by the hydrolyzed product again have short lifetimes, but the channels are distinctly different from those formed by the ester gramicidin A. Furthermore, well-behaved asymmetric channels form between the hydrolysis product and reference subunits that have either an L- or a D-residue at the formyl-NH-terminus.     

Functional asymmetry of transmembrane segments in nicotinic acetylcholine receptors

Nicotinic acetylcholine receptors are heteropentameric ion channels that open upon activation to a single conducting state. The second transmembrane segments of each subunit were identified as channel-forming elements, but their respective contribution in the gating process remains unclear. Moreover, the detailed impact of variations of the membrane potential, such as occurring during an action potential, on the transmembrane domains, is unknown. Residues at the 12′ position, close to the center of each second transmembrane segment, play a key role in channel gating. We examined their functional symmetry by substituting a lysine to that position of each subunit and measuring the electrical activity of single channels. For 12′ lysines in the α, γ and δ subunits rapid transitions between an intermediate and large conductance appeared, which are interpreted as single lysine protonation events. From the kinetics of these transitions we calculated the pK _a values of respective lysines and showed that they vary differently with membrane hyperpolarization. Respective mutations in β or ε subunits gave receptors with openings of either intermediate or large conductance, suggesting extreme pK _a values in two open state conformations. The results demonstrate that these parts of the highly homologous transmembrane domains, as probed by the 12′ lysines, sense unequal microenvironments and are differently affected by physiologically relevant voltage changes. Moreover, observation of various gating events for mutants of α subunits suggests that the open channel pore exists in multiple conformations, which in turn supports the notion of functional asymmetry of the channel.     

AtKC1 is a general modulator of Arabidopsis inward Shaker channel activity

A functional Shaker potassium channel requires assembly of four α-subunits encoded by a single gene or various genes from the Shaker family. In Arabidopsis thaliana, AtKC1, a Shaker α-subunit that is silent when expressed alone, has been shown to regulate the activity of AKT1 by forming heteromeric AtKC1-AKT1 channels. Here, we investigated whether AtKC1 is a general regulator of channel activity. Co-expression in Xenopus oocytes of a dominant negative (pore-mutated) AtKC1 subunit with the inward Shaker channel subunits KAT1, KAT2 or AKT2, or the outward subunits SKOR or GORK, revealed that the three inward subunits functionally interact with AtKC1 while the outward ones cannot. Localization experiments in plant protoplasts showed that KAT2 was able to re-locate AtKC1 fused to GFP from endomembranes to the plasma membrane, indicating that heteromeric AtKC1-KAT2 channels are efficiently targeted to the plasma membrane. Functional properties of heteromeric channels involving AtKC1 and KAT1, KAT2 or AKT2 were analysed by voltage clamp after co-expression of the respective subunits in Xenopus oocytes. AtKC1 behaved as a regulatory subunit within the heterotetrameric channel, reducing the macroscopic conductance and negatively shifting the channel activation potential. Expression studies showed that AtKC1 and its identified Shaker partners have overlapping expression patterns, supporting the hypothesis of a general regulation of inward channel activity by AtKC1 in planta. Lastly, AtKC1 disruption appeared to reduce plant biomass production, showing that AtKC1-mediated channel activity regulation is required for normal plant growth.     

Isolation of a single carboxyl-carboxylate proton binding site in the pore of a cyclic nucleotide-gated channel.

The pore of the catfish olfactory cyclic nucleotide-gated (CNG) channel contains four conserved glutamate residues, one from each subunit, that form a high-affinity binding site for extracellular divalent cations. Previous work showed that these residues form two independent and equivalent high-pKa (approximately 7.6) proton binding sites, giving rise to three pH-dependent conductance states, and it was suggested that the sites were formed by pairing of the glutamates into two independent carboxyl-carboxylates. To test further this physical picture, wild-type CNG subunits were coexpressed in Xenopus oocytes with subunits lacking the critical glutamate residue, and single channel currents through hybrid CNG channels containing one to three wild-type (WT) subunits were recorded. One of these hybrid channels had two pH-dependent conductance states whose occupancy was controlled by a single high-pKa protonation site. Expression of dimers of concatenated CNG channel subunits confirmed that this hybrid contained two WT and two mutant subunits, supporting the idea that a single protonation site is made from two glutamates (dimer expression also implied the subunit makeup of the other hybrid channels). Thus, the proton binding sites in the WT channel occur as a result of the pairing of two glutamate residues. This conclusion places these residues in close proximity to one another in the pore and implies that at any instant in time detailed fourfold symmetry is disrupted.     

The beta subunit increases the Ca2+ sensitivity of large conductance Ca2+-activated potassium channels by retaining the gating in the bursting states

Coexpression of the beta subunit (KV,Cabeta) with the alpha subunit of mammalian large conductance Ca2+- activated K+ (BK) channels greatly increases the apparent Ca2+ sensitivity of the channel. Using single-channel analysis to investigate the mechanism for this increase, we found that the beta subunit increased open probability (Po) by increasing burst duration 20-100-fold, while having little effect on the durations of the gaps (closed intervals) between bursts or on the numbers of detected open and closed states entered during gating. The effect of the beta subunit was not equivalent to raising intracellular Ca2+ in the absence of the beta subunit, suggesting that the beta subunit does not act by increasing all the Ca2+ binding rates proportionally. The beta subunit also inhibited transitions to subconductance levels. It is the retention of the BK channel in the bursting states by the beta subunit that increases the apparent Ca2+ sensitivity of the channel. In the presence of the beta subunit, each burst of openings is greatly amplified in duration through increases in both the numbers of openings per burst and in the mean open times. Native BK channels from cultured rat skeletal muscle were found to have bursting kinetics similar to channels expressed from alpha subunits alone.     

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.     

Subconductance states of single sodium channels modified by chloramine-T and sea anemone toxin in neuroblastoma cells

Single channel currents of chloramine-T (Chl-T) and sea anemone toxin (ATX-II) modified sodium channels were studied in neuroblastoma cells. With both substances similar subconductance states have been observed. The conductances of the sublevels were multiples of the unit step which was about onefourth of the most frequently occurring main conductance. Thus, the current levels observed were one fourth, half and five-fourths of the main current size. Both substances caused a slower decay of the averaged current compared to the current of the native channels. The main single-channel conductance was 15.2 pS (T=16°C) for the Chl-T and 10.8 pS (T=12°C) for the ATX-II modified channels. The channel open time was doubled by ATX-II, but was not increased significantly by Chl-T. The existence of the subconductance states suggests that the native channels may also have multiple open conformations.