Immobilizing the moving parts of voltage-gated ion channels

Voltage-gated ion channels have at least two classes of moving parts, voltage sensors that respond to changes in the transmembrane potential and gates that create or deny permeant ions access to the conduction pathway. To explore the coupling between voltage sensors and gates, we have systematically immobilized each using a bifunctional photoactivatable cross-linker, benzophenone-4-carboxamidocysteine methanethiosulfonate, that can be tethered to cysteines introduced into the channel protein by mutagenesis. To validate the method, we first tested it on the inactivation gate of the sodium channel. The benzophenone-labeled inactivation gate of the sodium channel can be trapped selectively either in an open or closed state by ultraviolet irradiation at either a hyperpolarized or depolarized voltage, respectively. To verify that ultraviolet light can immobilize S4 segments, we examined its relative effects on ionic and gating currents in Shaker potassium channels, labeled at residue 359 at the extracellular end of the S4 segment. As predicted by the tetrameric stoichiometry of these potassium channels, ultraviolet irradiation reduces ionic current by approximately the fourth power of the gating current reduction, suggesting little cooperativity between the movements of individual S4 segments. Photocross-linking occurs preferably at hyperpolarized voltages after labeling residue 359, suggesting that depolarization moves the benzophenone adduct out of a restricted environment. Immobilization of the S4 segment of the second domain of sodium channels prevents channels from opening. By contrast, photocross-linking the S4 segment of the fourth domain of the sodium channel has effects on both activation and inactivation. Our results indicate that specific voltage sensors of the sodium channel play unique roles in gating, and suggest that movement of one voltage sensor, the S4 segment of domain 4, is at least a two-step process, each step coupled to a different gate.     

Voltage clamp fluorimetry reveals a novel outer pore instability in a mammalian voltage-gated potassium channel

Voltage-gated potassium (Kv) channel gating involves complex structural rearrangements that regulate the ability of channels to conduct K(+) ions. Fluorescence-based approaches provide a powerful technique to directly report structural dynamics underlying these gating processes in Shaker Kv channels. Here, we apply voltage clamp fluorimetry, for the first time, to study voltage sensor motions in mammalian Kv1.5 channels. Despite the homology between Kv1.5 and the Shaker channel, attaching TMRM or PyMPO fluorescent probes to substituted cysteine residues in the S3-S4 linker of Kv1.5 (M394C-V401C) revealed unique and unusual fluorescence signals. Whereas the fluorescence during voltage sensor movement in Shaker channels was monoexponential and occurred with a similar time course to ionic current activation, the fluorescence report of Kv1.5 voltage sensor motions was transient with a prominent rapidly dequenching component that, with TMRM at A397C (equivalent to Shaker A359C), represented 36 +/- 3% of the total signal and occurred with a tau of 3.4 +/- 0.6 ms at +60 mV (n = 4). Using a number of approaches, including 4-AP drug block and the ILT triple mutation, which dissociate channel opening from voltage sensor movement, we demonstrate that the unique dequenching component of fluorescence is associated with channel opening. By regulating the outer pore structure using raised (99 mM) external K(+) to stabilize the conducting configuration of the selectivity filter, or the mutations W472F (equivalent to Shaker W434F) and H463G to stabilize the nonconducting (P-type inactivated) configuration of the selectivity filter, we show that the dequenching of fluorescence reflects rapid structural events at the selectivity filter gate rather than the intracellular pore gate.     

Movement of the S4 segment in the hERG potassium channel during membrane depolarization

Abstract

The hERG potassium channel is a member of the voltage gated potassium (Kv) channel family, comprising a pore domain and four voltage sensing domains (VSDs). Like other Kv channels, the VSD senses changes in membrane voltage and transmits the signal to gates located in the pore domain; the gates open at positive potentials (activation) and close at negative potentials, thereby controlling the ion flux. hERG, however, differs from other Kv channels in that it is activated slowly but inactivated rapidly – a property that is crucial for the role it plays in the repolarization of the cardiac action potential. Voltage-gating requires movement of gating charges across the membrane electric field, which is accomplished by the transmembrane movement of the fourth transmembrane segment, S4, of the VSD containing the positively charged arginine or lysine residues. Here we ask if the functional differences between hERG and other Kv channels could arise from differences in the transmembrane movement of S4. To address this, we have introduced single cysteine residues into the S4 region of the VSD, expressed the mutant channels in Xenopus oocytes and examined the effect of membrane impermeable para-chloromercuribenzene sulphonate on function by the two-electrode voltage clamp technique. Our results show that depolarization results in the accessibility of seven consecutive S4 residues, including the first two charged residues, K525 and R528, to extracellularly applied reagent. These data indicate that the extent of S4 movement in hERG is similar to other Kv channels, including the archabacterial KvAP and the Shaker channel of Drosophila.     

Gating charge immobilization caused by the transition between inactivated states in the Kv1.5 channel

Sustained Na(+) or Li(+) conductance is a feature of the inactivated state in wild-type (WT) and nonconducting Shaker and Kv1.5 channels, and has been used here to investigate the cause of off-gating charge immobilization in WT and Kv1.5-W472F nonconducting mutant channels. Off-gating immobilization in response to brief pulses in cells perfused with NMG/NMG is the result of a more negative voltage dependence of charge recovery (V(1/2) is -96 mV) compared with on-gating charge movement (V(1/2) is -6.3 mV). This shift is known to be associated with slow inactivation in Shaker channels and the disparity is reduced by 40 mV, or approximately 50% in the presence of 135 mM Cs. Off-gating charge immobilization is voltage-dependent with a V(1/2) of -12 mV, and correlates well with the development of Na(+) conductance on repolarization through C-type inactivated channels (V(1/2) is -11 mV). As well, the time-dependent development of the inward Na(+) tail current and gating charge immobilization after depolarizing pulses of different durations has the same time constant (tau = 2.7 ms). These results indicate that in Kv1.5 channels the transition to a stable C-type inactivated state takes only 2-3 ms and results in strong charge immobilization in the absence of Group IA metal cations, or even in the presence of Na. Inclusion of low concentrations of Cs delays the appearance of Na(+) tail currents in WT channels, prevents transition to inactivated states in Kv1.5-W472F nonconducting mutant channels, and removes charge immobilization. Higher concentrations of Cs are able to modulate the deactivating transition in Kv1.5 channels and prevent the residual slowing of charge return.     

Voltage sensitivity and gating charge in Shaker and Shab family potassium channels.

The members of the voltage-dependent potassium channel family subserve a variety of functions and are expected to have voltage sensors with different sensitivities. The Shaker channel of Drosophila, which underlies a transient potassium current, has a high voltage sensitivity that is conferred by a large gating charge movement, approximately 13 elementary charges. A Shaker subunit's primary voltage-sensing (S4) region has seven positively charged residues. The Shab channel and its homologue Kv2.1 both carry a delayed-rectifier current, and their subunits have only five positively charged residues in S4; they would be expected to have smaller gating-charge movements and voltage sensitivities. We have characterized the gating currents and single-channel behavior of Shab channels and have estimated the charge movement in Shaker, Shab, and their rat homologues Kv1.1 and Kv2.1 by measuring the voltage dependence of open probability at very negative voltages and comparing this with the charge-voltage relationships. We find that Shab has a relatively small gating charge, approximately 7.5 e(o). Surprisingly, the corresponding mammalian delayed rectifier Kv2.1, which has the same complement of charged residues in the S2, S3, and S4 segments, has a gating charge of 12.5 e(o), essentially equal to that of Shaker and Kv1.1. Evidence for very strong coupling between charge movement and channel opening is seen in two channel types, with the probability of voltage-independent channel openings measured to be below 10(-9) in Shaker and below 4 x 10(-8) in Kv2.1.     

S4 movement in a mammalian HCN channel

Hyperpolarization-activated, cyclic nucleotide-gated ion channels (HCN) mediate an inward cation current that contributes to spontaneous rhythmic firing activity in the heart and the brain. HCN channels share sequence homology with depolarization-activated Kv channels, including six transmembrane domains and a positively charged S4 segment. S4 has been shown to function as the voltage sensor and to undergo a voltage-dependent movement in the Shaker K+ channel (a Kv channel) and in the spHCN channel (an HCN channel from sea urchin). However, it is still unknown whether S4 undergoes a similar movement in mammalian HCN channels. In this study, we used cysteine accessibility to determine whether there is voltage-dependent S4 movement in a mammalian HCN1 channel. Six cysteine mutations (R247C, T249C, I251C, S253C, L254C, and S261C) were used to assess S4 movement of the heterologously expressed HCN1 channel in Xenopus oocytes. We found a state-dependent accessibility for four S4 residues: T249C and S253C from the extracellular solution, and L254C and S261C from the internal solution. We conclude that S4 moves in a voltage-dependent manner in HCN1 channels, similar to its movement in the spHCN channel. This S4 movement suggests that the role of S4 as a voltage sensor is conserved in HCN channels. In addition, to determine the reason for the different cAMP modulation and the different voltage range of activation in spHCN channels compared with HCN1 channels, we constructed a COOH-terminal-deleted spHCN. This channel appeared to be similar to a COOH-terminal-deleted HCN1 channel, suggesting that the main functional differences between spHCN and HCN1 channels are due to differences in their COOH termini or in the interaction between the COOH terminus and the rest of the channel protein in spHCN channels compared with HCN1 channels.     

Electrostatic model of S4 motion in voltage-gated ion channels

The S4 transmembrane domain of the family of voltage-gated ion channels is generally thought to be the voltage sensor, whose translocation by an applied electric field produces the gating current. Experiments on hSkMI Na(+) channels and both Shaker and EAG K(+) channels indicate which S4 residues cross the membrane-solution interface during activation gating. Using this structural information, we derive the steady-state properties of gating-charge transfer for wild-type and mutant Shaker K(+) channels. Assuming that the energetics of gating is dominated by electrostatic forces between S4 charges and countercharges on neighboring transmembrane domains, we calculate the total energy as a function of transmembrane displacement and twist of the S4 domain. The resulting electrostatic energy surface exhibits a series of deep energy minima, corresponding to the transition states of the gating process. The steady-state gating-charge distribution is then given by a Boltzmann distribution among the transition states. The resulting gating-charge distributions are compared to experimental results on wild-type and charge-neutralized mutants of the Shaker K(+) channel.     

Collapse of conductance is prevented by a glutamate residue conserved in voltage-dependent K(+) channels

Voltage-dependent K(+) channel gating is influenced by the permeating ions. Extracellular K(+) determines the occupation of sites in the channels where the cation interferes with the motion of the gates. When external [K(+)] decreases, some K(+) channels open too briefly to allow the conduction of measurable current. Given that extracellular K(+) is normally low, we have studied if negatively charged amino acids in the extracellular loops of Shaker K(+) channels contribute to increase the local [K(+)]. Surprisingly, neutralization of the charge of most acidic residues has minor effects on gating. However, a glutamate residue (E418) located at the external end of the membrane spanning segment S5 is absolutely required for keeping channels active at the normal external [K(+)]. E418 is conserved in all families of voltage-dependent K(+) channels. Although the channel mutant E418Q has kinetic properties resembling those produced by removal of K(+) from the pore, it seems that E418 is not simply concentrating cations near the channel mouth, but has a direct and critical role in gating. Our data suggest that E418 contributes to stabilize the S4 voltage sensor in the depolarized position, thus permitting maintenance of the channel open conformation.     

KCNE peptides differently affect voltage sensor equilibrium and equilibration rates in KCNQ1 K+ channels

KCNQ1 voltage-gated K(+) channels assemble with the family of KCNE type I transmembrane peptides to afford membrane-embedded complexes with diverse channel gating properties. KCNQ1/KCNE1 complexes generate the very slowly activating cardiac I(Ks) current, whereas assembly with KCNE3 produces a constitutively conducting complex involved in K(+) recycling in epithelia. To determine whether these two KCNE peptides influence voltage sensing in KCNQ1 channels, we monitored the position of the S4 voltage sensor in KCNQ1/KCNE complexes using cysteine accessibility experiments. A panel of KCNQ1 S4 cysteine mutants was expressed in Xenopus oocytes, treated with the membrane-impermeant cysteine-specific reagent 2-(trimethylammonium) ethyl methanethiosulfonate (MTSET), and the voltage-dependent accessibility of each mutant was determined. Of these S4 cysteine mutants, three (R228C, G229C, I230C) were modified by MTSET only when KCNQ1 was depolarized. We then employed these state-dependent residues to determine how assembly with KCNE1 and KCNE3 affects KCNQ1 voltage sensor equilibrium and equilibration rates. In the presence of KCNE1, MTSET modification rates for the majority of the cysteine mutants were approximately 10-fold slower, as was recently reported to indicate that the kinetics of the KCNQ1 voltage sensor are slowed by KCNE1 (Nakajo, K., and Y. Kubo. 2007 J. Gen. Physiol. 130:269-281). Since MTS modification rates reflect an amalgam of reagent accessibility, chemical reactivity, and protein conformational changes, we varied the depolarization pulse duration to determine whether KCNE1 slows the equilibration rate of the voltage sensors. Using the state-dependent cysteine mutants, we determined that MTSET modification rates were essentially independent of depolarization pulse duration. These results demonstrate that upon depolarization the voltage sensors reach equilibrium quickly in the presence of KCNE1 and the slow gating of the channel complex is not due to slowly moving voltage sensors. In contrast, all cysteine substitutions in the S4 of KCNQ1/KCNE3 complexes were freely accessible to MTSET independent of voltage, which is consistent with KCNE3 shifting the voltage sensor equilibrium to favor the active state at hyperpolarizing potentials. In total, these results suggest that KCNE peptides differently modulate the voltage sensor in KCNQ1 K(+) channels.     

Cross talk between activation and slow inactivation gates of Shaker potassium channels

This study addresses the energetic coupling between the activation and slow inactivation gates of Shaker potassium channels. To track the status of the activation gate in inactivated channels that are nonconducting, we used two functional assays: the accessibility of a cysteine residue engineered into the protein lining the pore cavity (V474C) and the liberation by depolarization of a Cs(+) ion trapped behind the closed activation gate. We determined that the rate of activation gate movement depends on the state of the inactivation gate. A closed inactivation gate favors faster opening and slower closing of the activation gate. We also show that hyperpolarization closes the activation gate long before a channel recovers from inactivation. Because activation and slow inactivation are ubiquitous gating processes in potassium channels, the cross talk between them is likely to be a fundamental factor in controlling ion flux across membranes.     

Voltage-dependent structural interactions in the Shaker K(+) channel

Using a strategy related to intragenic suppression, we previously obtained evidence for structural interactions in the voltage sensor of Shaker K(+) channels between residues E283 in S2 and R368 and R371 in S4 (Tiwari-Woodruff, S.K., C.T. Schulteis, A.F. Mock, and D. M. Papazian. 1997. Biophys. J. 72:1489-1500). Because R368 and R371 are involved in the conformational changes that accompany voltage-dependent activation, we tested the hypothesis that these S4 residues interact with E283 in S2 in a subset of the conformational states that make up the activation pathway in Shaker channels. First, the location of residue 283 at hyperpolarized and depolarized potentials was inferred by substituting a cysteine at that position and determining its reactivity with hydrophilic, sulfhydryl-specific probes. The results indicate that position 283 reacts with extracellularly applied sulfhydryl reagents with similar rates at both hyperpolarized and depolarized potentials. We conclude that E283 is located near the extracellular surface of the protein in both resting and activated conformations. Second, we studied the functional phenotypes of double charge reversal mutations between positions 283 and 368 and between 283 and 371 to gain insight into the conformations in which these positions approach each other most closely. We found that combining charge reversal mutations at positions 283 and 371 stabilized an activated conformation of the channel, and dramatically slowed transitions into and out of this state. In contrast, charge reversal mutations at positions 283 and 368 stabilized a closed conformation, which by virtue of the inferred position of 368 corresponds to a partially activated (intermediate) closed conformation. From these results, we propose a preliminary model for the rearrangement of structural interactions of the voltage sensor during activation of Shaker K(+) channels.     

Modes of operation of the BKCa channel beta2 subunit

The beta(2) subunit of the large conductance Ca(2+)- and voltage-activated K(+) channel (BK(Ca)) modulates a number of channel functions, such as the apparent Ca(2+)/voltage sensitivity, pharmacological and kinetic properties of the channel. In addition, the N terminus of the beta(2) subunit acts as an inactivating particle that produces a relatively fast inactivation of the ionic conductance. Applying voltage clamp fluorometry to fluorescently labeled human BK(Ca) channels (hSlo), we have investigated the mechanisms of operation of the beta(2) subunit. We found that the leftward shift on the voltage axis of channel activation curves (G(V)) produced by coexpression with beta(2) subunits is associated with a shift in the same direction of the fluorescence vs. voltage curves (F(V)), which are reporting the voltage dependence of the main voltage-sensing region of hSlo (S4-transmembrane domain). In addition, we investigated the inactivating mechanism of the beta(2) subunits by comparing its properties with the ones of the typical N-type inactivation process of Shaker channel. While fluorescence recordings from the inactivated Shaker channels revealed the immobilization of the S4 segments in the active conformation, we did not observe a similar feature in BK(Ca) channels coexpressed with the beta(2) subunit. The experimental observations are consistent with the view that the beta(2) subunit of BK(Ca) channels facilitates channel activation by changing the voltage sensor equilibrium and that the beta(2)-induced inactivation process does not follow a typical N-type mechanism.     

ATP-sensitive potassium channels and vascular function

Fluorescence-based approaches provide powerful techniques to directly report structural dynamics underlying gating processes in Shaker K_V channels. Here, following on from work carried out in Shaker channels, we have used voltage clamp fluorimetry for the first time to study voltage sensor motions in mammalian K_V1.5 channels, by attaching TMRM fluorescent probes to substituted cysteine residues in the S3-S4 linker of K_V1.5 (A397C). Compared with the Shaker channel, there are significant differences in the fluorescence signals that occur on activation of the channel. In addition to a well-understood fluorescence quenching signal associated with S4 movement, we have recorded a unique partial recovery of fluorescence after the quenching that is attributable to gating events at the outer pore mouth,¹ that is not seen in Shaker despite significant homology between it and Kv1.5 channels in the S5-P loop-S6 region. Extracellular potassium is known to modulate C-type inactivation in Shaker and K_V channels at sites in the outer pore mouth, and so here we have measured the concentration-dependence of potassium effects on the fluorescence recovery signals from A397C. Elevation of extracellular K⁺ inhibits the rapid fluorescence recovery, with complete abolition at 99 mM K⁺, and an IC₅₀ of 29 mM K⁺_o. These experiments suggest that the rapid fluorescence recovery reflects early gating movements associated with inactivation, modulated by extracellular K⁺, and further support the idea that outer pore motions occur rapidly after K_V1.5 channel opening and can be observed by fluorophores attached to the S3-S4 linker.     

A novel current pathway parallel to the central pore in a mutant voltage-gated potassium channel

Voltage-gated potassium channels are proteins composed of four subunits consisting of six membrane-spanning segments S1-S6, with S4 as the voltage sensor. The region between S5 and S6 forms the potassium-selective ion-conducting central α-pore. Recent studies showed that mutations in the voltage sensor of the Shaker channel could disclose another ion permeation pathway through the voltage-sensing domain (S1-S4) of the channel, the ω-pore. In our studies we used the voltage-gated hKv1.3 channel, and the insertion of a cysteine at position V388C (Shaker position 438) generated a current through the α-pore in high potassium outside and an inward current at hyperpolarizing potentials carried by different cations like Na(+), Li(+), Cs(+), and NH(4)(+). The observed inward current looked similar to the ω-current described for the R1C/S Shaker mutant channel and was not affected by some pore blockers like charybdotoxin and tetraethylammonium but was inhibited by a phenylalkylamine blocker (verapamil) that acts from the intracellular side. Therefore, we hypothesize that the hKv1.3_V388C mutation in the P-region generated a channel with two ion-conducting pathways. One, the α-pore allowing K(+) flux in the presence of K(+), and the second pathway, the σ-pore, functionally similar but physically distinct from the ω-pathway. The entry of this new pathway (σ-pore) is presumably located at the backside of Y395 (Shaker position 445), proceeds parallel to the α-pore in the S6-S6 interface gap, ending between S5 and S6 at the intracellular side of one α-subunit, and is blocked by verapamil.     

Mutations in the S4 region isolate the final voltage-dependent cooperative step in potassium channel activation

Charged residues in the S4 transmembrane segment play a key role in determining the sensitivity of voltage-gated ion channels to changes in voltage across the cell membrane. However, cooperative interactions between subunits also affect the voltage dependence of channel opening, and these interactions can be altered by making substitutions at uncharged residues in the S4 region. We have studied the activation of two mutant Shaker channels that have different S4 amino acid sequences, ILT (V369I, I372L, and S376T) and Shaw S4 (the S4 of Drosophila Shaw substituted into Shaker), and yet have very similar ionic current properties. Both mutations affect cooperativity, making a cooperative transition in the activation pathway rate limiting and shifting it to very positive voltages, but analysis of gating and ionic current recordings reveals that the ILT and Shaw S4 mutant channels have different activation pathways. Analysis of gating currents suggests that the dominant effect of the ILT mutation is to make the final cooperative transition to the open state of the channel rate limiting in an activation pathway that otherwise resembles that of Shaker. The charge movement associated with the final gating transition in ILT activation can be measured as an isolated component of charge movement in the voltage range of channel opening and accounts for 13% ( approximately 1.8 e0) of the total charge moved in the ILT activation pathway. The remainder of the ILT gating charge (87%) moves at negative voltages, where channels do not open, and confirms the presence of Shaker-like conformational changes between closed states in the activation pathway. In contrast to ILT, the activation pathway of Shaw S4 seems to involve a single cooperative charge-moving step between a closed and an open state. We cannot detect any voltage-dependent transitions between closed states for Shaw S4. Restoring basic residues that are missing in Shaw S4 (R1, R2, and K7) rescues charge movement between closed states in the activation pathway, but does not alter the voltage dependence of the rate-limiting transition in activation.     

Gating currents in Shaker K+ channels. Implications for activation and inactivation models.

We have studied ionic and gating currents in mutant and wild-type Shaker K+ channels to investigate the mechanisms of channel activation and the relationship between the voltage sensor of the channel and its inactivation particle. The turn on of the gating current shows a rising phase, indicating that the hypothetical identical activation subunits are not independent. Hyperpolarizing prepulses indicate that most of the voltage-dependence occurs in the transitions between closed states. The open-to-closed transition is voltage independent, as suggested by the presence of a rising phase in the off gating currents. In Shaker channels showing fast inactivation, the off gating charge is partially immobilized as a result of depolarizing pulses that elicit inactivation. In mutant channels lacking inactivation, the charge is recovered quickly at the end of the pulse. Internal TEA mimics the inactivation particle in its behavior but the charge immobilization is established faster and is complete. We conclude that the activation mechanism cannot be due to the movement of identical independent gating subunits, each undergoing first order transitions, and that the inactivation particle is responsible for charge immobilization in this channel.     

The contribution of individual subunits to the coupling of the voltage sensor to pore opening in Shaker K channels: effect of ILT mutations in heterotetramers

Voltage-gated ion channels couple conformational change(s) of the voltage-sensing domain to those of the opening of an intracellular gate to allow ionic conduction. Much larger positive potentials are required to couple these conformational changes to the opening of the gate of Shaker K(+) channels with the concurrent mutations V369I, I372L, and S376T (ILT) at the N-terminal end of the S4 segment. We used cut-open oocyte voltage clamp to study the biophysical and thermodynamical properties of heterotetrameric concatemerized channels with different stoichiometries of ILT mutations. The voltage-sensing domains of ILT mutant channels require smaller depolarization to activate but their intracellular gate does not immediately follow the movement of the voltage-sensing domain, requiring larger depolarization to open. Our results demonstrate that each subunit contributes equally to the rightward shift of the conductance-voltage relationship and that a single ILT-containing subunit is sufficient to induce a large enthalpic and entropic barrier, limiting opening of the intracellular gate.     

Energetics of pore opening in a voltage-gated K(+) channel

Voltage-dependent gating in K(+) channels results from the mechanical coupling of voltage sensor movements to pore opening. We used single and double mutations in the pore of the Shaker K(+) channel to analyze a late concerted pore opening transition and interpreted the results in the context of known K(+) channel structures. Gating sensitive mutations are located at mechanistically informative regions of the pore and are coupled energetically across distances up to 15 A. We propose that the pore is intrinsically more stable when closed, and that to open the pore the voltage sensors must exert positive work by applying an outward lateral force near the inner helix bundle.     

Localization of the extracellular end of the voltage sensor S4 in a potassium channel

The opening and closing of the pore of voltage-gated ion channels is the basis for the nervous impulse. These conformational changes are triggered by the movement of an intrinsic voltage sensor, the fourth transmembrane segment, S4. The central problem of how the movement of S4 is coupled to channel opening and where S4 is located in relation to the pore is still unsolved. Here, we estimate the position of the extracellular end of S4 in the Shaker potassium channel by analyzing the electrostatic effect of introduced charges in the pore-forming motif (S5-S6). We also present a three-dimensional model for all transmembrane segments. Knowledge of this structure is essential for the attempts to understand how voltage opens these channels.     

Charge movement in gating-locked HCN channels reveals weak coupling of voltage sensors and gate

HCN (hyperpolarization-activated cyclic nucleotide gated) pacemaker channels have an architecture similar to that of voltage-gated K⁺ channels, but they open with the opposite voltage dependence. HCN channels use essentially the same positively charged voltage sensors and intracellular activation gates as K⁺ channels, but apparently these two components are coupled differently. In this study, we examine the energetics of coupling between the voltage sensor and the pore by using cysteine mutant channels for which low concentrations of Cd²⁺ ions freeze the open–closed gating machinery but still allow the sensors to move. We were able to lock mutant channels either into open or into closed states by the application of Cd²⁺ and measure the effect on voltage sensor movement. Cd²⁺ did not immobilize the gating charge, as expected for strict coupling, but rather it produced shifts in the voltage dependence of voltage sensor charge movement, consistent with its effect of confining transitions to either closed or open states. From the magnitude of the Cd²⁺-induced shifts, we estimate that each voltage sensor produces a roughly three- to sevenfold effect on the open–closed equilibrium, corresponding to a coupling energy of ∼1.3–2 kT per sensor. Such coupling is not only opposite in sign to the coupling in K⁺ channels, but also much weaker.