Comparing the Temperature-Dependent Conductance of the Two Structurally Similar E. coli Porins OmpC and OmpF

The temperature-dependent ion conductance of OmpC, a major outer membrane channel of Escherichia coli, is predicted using all-atom molecular dynamics simulations and experimentally verified. To generalize previous results, OmpC is compared to its structural homolog OmpF at different KCl concentrations, pH values, and a broad temperature range. At low salt concentrations and up to room temperature, the molecular modeling predicts the experimental conductance accurately. At high salt concentrations above 1 M KCl and above room temperature, the simulations underestimate the conductance. Moreover, the temperature dependence of the channel conductance is different from that of the bulk, both in experiment and simulation, indicating a strong contribution of surface effects to the ion conductance. With respect to OmpC, subconductance levels can be observed in experiments only. Subconductance and gating levels can be clearly distinguished by their differences in conductance values and temperature-dependent behavior. With increasing temperature, the probability of a subconductance state to occur, increases, while the dwell time is decreased. The open probability, frequency, and dwell time of such states is largely pH- and KCl concentration-independent, while their amplitudes show a lower increase with increasing salt concentration than gating amplitudes. Voltage dependence of subconductance has been found to be negligible within the uncertainty of the measurements.     

Gating Kinetics of E. coli Poly-3-Hydroxybutyrate/Polyphosphate Channels in Planar Bilayer Membranes

Nonproteinaceous calcium channel complexes from Escherichia coli, composed of poly-(R)-3-hydroxybutyrate (PHB) and inorganic polyphosphate (polyP), exhibit two distinct gating modes (modes 1 and 2) in planar lipid bilayers. Here we report the kinetic characterization of the channel in mode 2, a mode characterized by two well-defined conductance levels, a fully open state (87 ± 3 pS), and a major subconductance state (56 ± 2 pS). Other subconductance states and full closures are rare (<0.5% of total time). Several kinetic properties of the channel showed asymmetric voltage-dependence indicating an asymmetry in the channel structure. Accordingly, single channels responded to potential change in one of two mirror-image patterns, postulated to arise from opposite orientations of the asymmetrical channel complex in the bilayer. The fraction of time spent in each conductance level was strongly voltage-sensitive. For channels reported in this study, presumably all oriented in the same direction, residence time in the fully open state increased as clamping potentials became more positive whereas residence time in the major subconductance state increased at more negative potentials. Analysis of open time distributions revealed existence of two kinetically distinct states for each level. The shorter time constants for both conductance states exhibited weak voltage-sensitivity; however, the longer time constants were strongly voltage-sensitive. A kinetic scheme, consistent with the complex voltage dependence of the channel, is proposed. Received: 1 February 1999/Revised: 2 April 1999     

Subconductance states in OmpF gating

Discrepancies were noted in the published conductance of the Escherichia coli porin OmpF. Results from various papers are hard to compare because of the use of different channel preparations, salt types and concentrations, and electrophysiological techniques (black lipid membrane (BLM) vs. patch clamp). To reconcile these data, we present a side-by-side comparison of OmpF activity studied with the two techniques on the same preparation of pure protein, and in the same low salt concentrations (150 mM KCl). The novel aspect of OmpF porin behavior revealed by this comparison is the ubiquitous existence of states of smaller conductance than the monomeric conductance (subconductance states), regardless of the techniques or experimental conditions used, and the drastic enhancement of subconductance gating by polyamines. Transitions to subconductance states have received little attention in previous publications, in particular when BLM electrophysiology was used. Monomeric closures are rare in recordings at clamped potentials, at least at voltages lower than ∼100-120 mV. Most closing activity is in the form of subconductance gating, which becomes more dominant in the presence of spermine, with a more frequent and prolonged occupation of these substates. A discussion of the molecular basis for this hallmark behavior of porin is presented.     

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.     

Slow conversions among subconductance states of cystic fibrosis transmembrane conductance regulator chloride channel.

The cystic fibrosis transmembrane conductance regulator (CFTR) chloride channel exhibits multiple subconductance states. To study the regulation of conductance states of the CFTR channel, we expressed the wild-type CFTR protein in HEK 293 cells, and isolated microsomal membrane vesicles for reconstitution studies in lipid bilayer membranes. A single CFTR channel had a dominant conductance of 7.8 pS (H), plus two sub-open states with conductances of approximately 6 pS (M) and 2.7 pS (L) in 200 mM KCl with 1 mM MgCl2 (intracellular) and 50 mM KCl with no MgCl2 (extracellular), with pH maintained at 7.4 by 10 mM HEPES-Tris on both sides of the channel. In 200 mM KCl, both H and L states could be measured in stable single-channel recordings, whereas M could not. Spontaneous transitions between H and L were slow; it took 4.5 min for L-->H, and 3.2 min for H-->L. These slow conversions among subconductance states of the CFTR channel were affected by extracellular Mg; in the presence of millimolar Mg, the channel remained stable in the H state. Similar phenomena were also observed with endogenous CFTR channels in T84 cells. In high-salt conditions (1.5 M KCl), all three conductance states of the expressed CFTR channel, 12.1 pS, 8.2 pS, and 3.6 pS, became stable and seemed to gate independently from each other. The existence of multiple stable conductance states associated with the CFTR channel suggests two possibilities: either a single CFTR molecule can exist in multiple configurations with different conductance values, or the CFTR channel may contain multimers of the 170-kDa CFTR protein, and different conductance states are due to different aggregation states of the CFTR protein.     

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.     

Batrachotoxin-modified sodium channels in planar lipid bilayers. Ion permeation and block

Batrachotoxin-modified, voltage-dependent sodium channels from canine forebrain were incorporated into planar lipid bilayers. Single-channel conductances were studied for [Na+] ranging between 0.02 and 3.5 M. Typically, the single-channel currents exhibited a simple two-state behavior, with transitions between closed and fully open states. Two other conductance states were observed: a subconductance state, usually seen at [NaCl] greater than or equal to 0.5 M, and a flickery state, usually seen at [NaCl] less than or equal to 0.5 M. The flickery state became more frequent as [NaCl] was decreased below 0.5 M. The K+/Na+ permeability ratio was approximately 0.16 in 0.5 and 2.5 M salt, independent of the Na+ mole fraction, which indicates that there are no interactions among permeant ions in the channels. Impermeant and permeant blocking ions (tetraethylammonium, Ca++, Zn++, and K+) have different effects when added to the extracellular and intracellular solutions, which indicates that the channel is asymmetrical and has at least two cation-binding sites. The conductance vs. [Na+] relation saturated at high concentrations, but could not be described by a Langmuir isotherm, as the conductance at low [NaCl] is higher than predicted from the data at [NaCl] greater than or equal to 1.0 M. At low [NaCl] (less than or equal to 0.1 M), increasing the ionic strength by additions of impermeant monovalent and divalent cations reduced the conductance, as if the magnitude of negative electrostatic potentials at the channel entrances were reduced. The conductances were comparable for channels in bilayers that carry a net negative charge and bilayers that carry no net charge. Together, these results lead to the conclusion that negative charges on the channel protein near the channel entrances increase the conductance, while lipid surface charges are less important.     

Multiple conductance states of the acetylcholine receptor channel complex

The acetylcholine-activated channel of vertebrate skeletal muscle, as manifested in cultured, developing cells, is able to adopt more than one conductance state. This paper briefly reviews the evidence for such multiple conductance channels and presents results showing that the amplitude of subconductance states does not depend on agonist size and (or) valence. This seems to rule out the possibility that subconductances occur during partial occlusion of the channel (by agonist molecules) and supports the idea that subconductances represent discrete, allosterically activated channel conformations.     

Single-channel currents from acetylcholine receptors in embryonic chick muscle. Kinetic and conductance properties of gaps within bursts

In tissue-cultured chick muscle, bursts of current from single nicotinic ion channels contain a variety of low-conductance gaps. One population has a lifetime of approximately 0.1 ms and an unknown conductance. A second population has a lifetime of 2-10 ms and conductance of zero. The third population has a lifetime of 0.5-1 ms and a mean conductance approximately 2% that of the main conductance state. This subconductance state has an agonist-dependent lifetime, longer for suberyldicholine than for acetylcholine, and is liganded to the same extent as the main conductance state. Subconductance gaps have a linear current-voltage behavior in the range -60 to -140 mV and appear to have the same reversal potential as the main state. The subconductance state is composed of a group of states which interconvert with correlation times longer than 300 microseconds.     

Regulation of TRPV5 Single-Channel Activity by Intracellular pH

The transient receptor potential channel TRPV5 contributes to the apical entry pathway for transcellular calcium reabsorption in the kidney. Acid load causes hypercalciuria in animals and humans. We have previously reported that intracellular protons directly inhibit TRPV5. Here, we examined the effects of intracellular pH on single-channel activity of TRPV5. We found that TRPV5 channels exhibit full and subconductance open states in excised inside–out patches of Chinese hamster ovary cells. The slope conductance values (Na⁺ as a charge carrier, between −25 and −75 mV) for full and subconductance opening at intracellular pH 7.4 were 59 ± 6 and 29 ± 3 pS, respectively. Intracellular acidification caused a small decrease in single-channel conductance. Importantly, intracellular acidification decreased open probability for the full and subconductance states and increased probability for closing. To investigate how intracellular protons decrease open probability of the channel, we proposed a simple three-state model for open–subconductance–closed state transition and examined the effects of acidification on the respective forward and reverse rate constants. We found that intracellular acidification decreases opening of TRPV5 predominantly by promoting a transition from the subconductance to the closed state. Thus, intracellular acidification directly inhibits TRPV5 by causing a conformational change(s) leading to a decrease of open probability of TRPV5 as well as of the single-channel conductance. Seung-Kuy Cha and Wasey Jabbar contributed equally to this work.     

Cysteine residues in the nucleotide binding domains regulate the conductance state of CFTR channels

Gating of cystic fibrosis transmembrane conductance regulator (CFTR) channels requires intermolecular or interdomain interactions, but the exact nature and physiological significance of those interactions remains uncertain. Subconductance states of the channel may result from alterations in interactions among domains, and studying mutant channels enriched for a single conductance type may elucidate those interactions. Analysis of CFTR channels in inside-out patches revealed that mutation of cysteine residues in NBD1 and NBD2 affects the frequency of channel opening to the full-size versus a 3-pS subconductance. Mutating cysteines in NBD1 resulted in channels that open almost exclusively to the 3-pS subconductance, while mutations of cysteines in NBD2 decreased the frequency of subconductance openings. Wild-type channels open to both size conductances and make fast transitions between them within a single open burst. Full-size and subconductance openings of both mutant and wild-type channels are similarly activated by ATP and phosphorylation. However, the different size conductances open very differently in the presence of a nonhydrolyzable ATP analog, with subconductance openings significantly shortened by ATPgammaS, while full-size channels are locked open. In wild-type channels, reducing conditions increase the frequency and decrease the open time of subconductance channels, while oxidizing conditions decrease the frequency of subconductance openings. In contrast, in the cysteine mutants studied, altering redox potential has little effect on gating of the subconductance.     

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.     

Subconductance states in calcium-activated potassium channels from canine airway smooth muscle

The single-channel patch clamp technique was used to analyze subconductance states in the 260 pS calcium-activated potassium channel from canine airway smooth muscle. More than sixty minutes of single channel data (greater than 87,000 events) from five excised patches were analyzed. Six subconductance amplitudes were clearly established to be 17, 33, 41, 52, 63 and 72% of the full conductance. Subconductance openings were usually brief (milliseconds) and represented less than 5% of the total channel open time, but they also persisted for several seconds on rare occasions. They appeared to be unaffected by voltage or time after seal formation, but may have increased in occurrence with decreasing calcium concentration. Irregular amplitude intervals, and the presence of ramp-like, analog transitions between conductance states, suggest a model for maxi-K subconductance states in which the channel protein undergoes random conformational changes causing a variable pore size.     

Selectivity Changes during Activation of Mutant Shaker Potassium Channels

Mutations of the pore-region residue T442 in Shaker channels result in large effects on channel kinetics. We studied mutations at this position in the backgrounds of NH₂-terminal–truncated Shaker H4 and a Shaker -NGK2 chimeric channel having high conductance (Lopez, G.A., Y.N. Jan, and L.Y. Jan. 1994. Nature (Lond.). 367: 179–182). While mutations of T442 to C, D, H, V, or Y resulted in undetectable expression in Xenopus oocytes, S and G mutants yielded functional channels having deactivation time constants and channel open times two to three orders of magnitude longer than those of the parental channel. Activation time courses at depolarized potentials were unaffected by the mutations, as were first-latency distributions in the T442S chimeric channel. The mutant channels show two subconductance levels, 37 and 70% of full conductance. From single-channel analysis, we concluded that channels always pass through the larger subconductance state on the way to and from the open state. The smaller subconductance state is traversed in ∼40% of activation time courses. These states apparently represent kinetic intermediates in channel gating having voltage-dependent transitions with apparent charge movements of ∼1.6 e₀. The fully open T442S chimeric channel has the conductance sequence Rb⁺ > NH₄ ⁺ > K⁺. The opposite conductance sequence, K⁺ > NH₄ ⁺ > Rb⁺, is observed in each of the subconductance states, with the smaller subconductance state discriminating most strongly against Rb⁺.     

Two Salt Bridges Differentially Contribute to the Maintenance of Cystic Fibrosis Transmembrane Conductance Regulator (CFTR) Channel Function

Previous studies have identified two salt bridges in human CFTR chloride ion channels, Arg³⁵²-Asp⁹⁹³ and Arg³⁴⁷-Asp⁹²⁴, that are required for normal channel function. In the present study, we determined how the two salt bridges cooperate to maintain the open pore architecture of CFTR. Our data suggest that Arg³⁴⁷ not only interacts with Asp⁹²⁴ but also interacts with Asp⁹⁹³. The tripartite interaction Arg³⁴⁷-Asp⁹²⁴-Asp⁹⁹³ mainly contributes to maintaining a stable s2 open subconductance state. The Arg³⁵²-Asp⁹⁹³ salt bridge, in contrast, is involved in stabilizing both the s2 and full (f) open conductance states, with the main contribution being to the f state. The s1 subconductance state does not require either salt bridge. In confirmation of the role of Arg³⁵² and Asp⁹⁹³, channels bearing cysteines at these sites could be latched into a full open state using the bifunctional cross-linker 1,2-ethanediyl bismethanethiosulfonate, but only when applied in the open state. Channels remained latched open even after washout of ATP. The results suggest that these interacting residues contribute differently to stabilizing the open pore in different phases of the gating cycle.     

Subconductance Gating and Voltage Sensitivity of Sarcoplasmic Reticulum K+ Channels: A Modeling Approach

Sarcoplasmic reticulum (SR) K⁺ channels are voltage-regulated channels that are thought to be actively gating when the membrane potential across the SR is close to zero as is expected physiologically. A characteristic of SR K⁺ channels is that they gate to subconductance open states but the relevance of the subconductance events and their contribution to the overall current flowing through the channels at physiological membrane potentials is not known. We have investigated the relationship between subconductance and full conductance openings and developed kinetic models to describe the voltage sensitivity of channel gating. Because there may be two subtypes of SR K⁺ channels (TRIC-A and TRIC-B) present in most tissues, to conduct our study on a homogeneous population of SR K⁺ channels, we incorporated SR vesicles derived from Tric-a knockout mice into artificial membranes to examine the remaining SR K⁺ channel (TRIC-B) function. The channels displayed very low open probability (Po) at negative potentials (≤0 mV) and opened predominantly to subconductance open states. Positive holding potentials primarily increased the frequency of subconductance state openings and thereby increased the number of subsequent transitions into the full open state, although a slowing of transitions back to the sublevels was also important. We investigated whether the subconductance gating could arise as an artifact of incomplete resolution of rapid transitions between full open and closed states; however, we were not able to produce a model that could fit the data as well as one that included multiple distinct current amplitudes. Our results suggest that the apparent subconductance openings will provide most of the K⁺ flux when the SR membrane potential is close to zero. The relative contribution played by openings to the full open state would increase if negative charge developed within the SR thus increasing the capacity of the channel to compensate for ionic imbalances.     

Sodium channel subconductance levels measured with a new variance-mean analysis

The currents through single Na+ channels were recorded from dissociated cells of the flexor digitorum brevis muscle of the mouse. At 15 degrees C the prolonged bursts of Na+ channel openings produced by application of the drug DPI 201-106 had brief sojourns to subconductance levels. The subconductance events were relatively rare and brief, but could be identified using a new technique that sorts amplitude estimates based on their variance. The resulting "levels histogram" had a resolution of the conductance levels during channel activity that was superior to that of standard amplitude histograms. Cooling the preparation to 0 degrees C prolonged the subconductance events, and permitted further quantitative analysis of their amplitudes, as well as clear observations of single-channel subconductance events from untreated Na+ channels. In all cases the results were similar: a subconductance level, with an amplitude of roughly 35% of the fully open conductance and similar reversal potential, was present in both drug-treated and normal Na+ channels. Drug-treated channels spent approximately 3-6% of their total open time in the subconductance state over a range of potentials that caused the open probability to vary between 0.1 and 0.9. The summed levels histograms from many channels had a distinctive form, with broader, asymmetrical open and substate distributions compared with those of the closed state. Individual subconductance events to levels other than the most common 35% were also observed. I conclude that subconductance events are a normal subset of the open state of Na+ channels, whether or not they are drug treated. The subconductance events may represent a conformational alteration of the channel that occurs when it conducts ions.     

Examination of subconductance levels arising from a single ion channel.

Single-channel records often show frequent currents at a main conductance level and occasional currents at subconductance levels. In some instances, the conductances occur at regular levels that are multiples of a minimum conductance. It is well-appreciated that multiple conductance levels may arise either from the co-operative gating of more than one pore or from changes that occur in a single pore. In this paper, we used theoretical models of ion permeation to examine subconductances arising in a single-pore channel. In particular, the work focuses on the following question: how can an ion channel that provides only one aqueous pore through the membrane produce regular subconductances and a main conductance that all have the same selectivity and the same ion binding affinity? The three types of ion permeation models used in this study showed that a single-pore channel can have subconductances because of long-lived conformational states, because of alterations in rapid fluctuations between conformational states, or because of slight alterations in the electrostatic properties in the channel's entrance vestibules. Regular subconductances with the same selectivity and binding affinity can arise in a single pore even if the energy profile changes do not meet the constant peak offset condition. The results show that the appearance of regular subconductance levels in a single-channel recording is not sufficient evidence to conclude that identical pores have co-operative gating, as would arise in a channel that is a multi-pore complex.     

Determination of the functional unit of the cystic fibrosis transmembrane conductance regulator chloride channel. One polypeptide forms one pore

The magnitudes and distributions of subconductance states were studied in chloride channels formed by the wild-type cystic fibrosis transmembrane conductance regulator (CFTR) and in CFTRs bearing amino acid substitutions in transmembrane segment 6. Within an open burst, it was possible to distinguish three distinct conductance states referred to as the full conductance, subconductance 1, and subconductance 2 states. Amino acid substitutions in transmembrane segment 6 altered the duration and probability of occurrence of these subconductance states but did not greatly alter their relative amplitudes. Results from real time measurements indicated that covalent modification of single R334C-CFTR channels by [2-(trimethylammonium)ethyl]methanethiosulfonate resulted in the simultaneous modification of all three conductance levels in what appeared to be a single step, without changing the proportion of time spent in each state. This behavior suggests that at least a portion of the conduction path is common to all three conducting states. The time course for the modification of R334C-CFTR, measured in outside-out macropatches using a rapid perfusion system, was also consistent with a single modification step as if each pore contained only a single copy of the cysteine at position 334. These results are consistent with a model for the CFTR conduction pathway in which a single anion-conducting pore is formed by a single CFTR polypeptide.     

K channel subconductance levels result from heteromeric pore conformations

Voltage-gated K channels assemble from four identical subunits symmetrically arranged around a central permeation pathway. Each subunit harbors a voltage-sensing domain. The sigmoidal nature of the activation kinetics suggests that multiple sensors need to undergo a conformational change before the channel can open. Following activation, individual K channels alternate stochastically between two main permeation states, open and closed. This binary character of single channel behavior suggests the presence of a structure in the permeation pathway that can exist in only two conformations. However, single channel analysis of drk1 (K(v)2.1) K channels demonstrated the existence of four additional, intermediate conductance levels. These short-lived subconductance levels are visited when the channel gate moves between the closed and fully open state. We have proposed that these sublevels arise from transient heteromeric pore conformations, in which some, but not all, subunits are in the "open" state. A minimal model based on this hypothesis relates specific subconductance states with the number of activated subunits (Chapman et al., 1997). To stringently test this hypothesis, we constructed a tandem dimer that links two K channel subunits with different activation thresholds. Activation of this dimer by strong depolarizations resulted in the characteristic binary open-close behavior. However, depolarizations to membrane potentials in between the activation thresholds of the two parents elicited highly unusual single channel gating, displaying frequent visits to two subconductance levels. The voltage dependence and kinetics of the small and large sublevels associate them with the activation of one and two subunits, respectively. The data therefore support the hypothesis that subconductance levels result from heteromeric pore conformations. In this model, both sensor movement and channel opening have a subunit basis and these processes are allosterically coupled.