Effect of charge,topology and orientation of the electric field on the interaction of peptides with the α‐hemolysin pore

Nanopore analysis is an emerging technique of structural biology which employs nanopores, such as the α‐hemolysin pore, as a biosensor. A voltage applied across a membrane containing a nanopore generates a current, which is partially blocked when a molecule interacts with the pore. The magnitude (I) and the duration (T) of the current blockade provide an event signature for that molecule. Two peptides, CY12(+)T1 and CY12(?)T1 with net charges + 2 and ? 2, respectively, were analysed using different applied voltages and all four possible orientations of the electrodes and pore. The four orientations were vestibule downstream (VD), vestibule upstream (VU), stem downstream (SD) and stem upstream (SU) where vestibule and stem refer to the side of the pore on which the peptide was placed and downstream and upstream refer to the application of a positive or negative electrophoretic force, respectively. For CY12(+)T1, the effect of voltage on the event duration was consistent with translocation in the VD and SD configurations, but only intercalation events were observed in the VU and SU configurations. For CY12(?)T1, translocations were only observed in the VD and VU configurations. The results are interpreted in terms of two energy barriers on either side of the lumen of the pore. The difference in height of the barriers determines the preferred direction of exit. Electroosmotic flow and current rectification due to the pore as well as the dipole moment and charge of the peptide also play significant roles. Thus, factors other than simple electrophoresis are important for determining the interaction of small peptides with the pore. Copyright © 2011 European Peptide Society and John Wiley & Sons, Ltd.     

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.     

Amphiphilic Blockers Punch through a Mutant CLC-0 Pore

Intracellularly applied amphiphilic molecules, such as p-chlorophenoxy acetate (CPA) and octanoate, block various pore-open mutants of CLC-0. The voltage-dependent block of a particular pore-open mutant, E166G, was found to be multiphasic. In symmetrical 140 mM Cl⁻, the apparent affinity of the blocker in this mutant increased with a negative membrane potential but, paradoxically, decreased when the negative membrane potential was greater than −80 mV, a phenomenon similar to the blocker “punch-through” shown in many blocker studies of cation channels. To provide further evidence of the punch-through of CPA and octanoate, we studied the dissociation rate of the blocker from the pore by measuring the time constant of relief from the block under various voltage and ionic conditions. Consistent with the voltage dependence of the effect on the steady-state current, the rate of CPA dissociation from the E166G pore reached a minimum at −80 mV in symmetrical 140 mM Cl⁻, and the direction of current recovery suggested that the bound CPA in the pore can dissociate into both intracellular and extracellular solutions. Moreover, the CPA dissociation depends upon the Cl⁻ reversal potential with a minimal dissociation rate at a voltage 80 mV more negative than the Cl⁻ reversal potential. That the shift of the CPA-dissociation rate follows the Cl⁻ gradient across the membrane argues that these blockers can indeed punch through the channel pore. Furthermore, a minimal CPA-dissociation rate at a voltage 80 mV more negative than the Cl⁻ reversal potential suggests that the outward blocker movement through the CLC-0 pore is more difficult than the inward movement.     

Properties of deactivation gating currents in Shaker channels

The charge versus voltage relation of voltage-sensor domains shifts in the voltage axis depending on the initial voltage. Here we show that in nonconducting W434F Shaker K⁺ channels, a large portion of this charge-voltage shift is apparent due to a dramatic slowing of the deactivation gating currents, Ig_D (with τ up to 80 ms), which develops with a time course of ∼1.8 s. This slowing in Ig_D adds up to the slowing due to pore opening and is absent in the presence of 4-aminopyridine, a compound that prevents the last gating step that leads to pore opening. A remaining 10–15 mV negative shift in the voltage dependence of both the kinetics and the charge movement persists independently of the depolarizing prepulse duration and remains in the presence of 4-aminopyridine, suggesting the existence of an intrinsic offset in the local electric field seen by activated channels. We propose a new (to our knowledge) kinetic model that accounts for these observations.     

Nanopore analysis of tethered peptides

Peptides of 12 amino acids were tethered via a terminal cysteine to mono‐, di‐, tri‐, and tetrabromomethyl‐substituted benzene to produce bundles of one to four peptide strands (CY12‐T1 to CY12‐T4, respectively). The interaction of the bundles with the α‐hemolysin pore was assessed by measuring the blockade currents (I) and times (T) at an applied potential of ? 50, ? 100, and ? 150 mV. Three types of events could be distinguished: bumping events, with small I and short T where the molecule transiently interacts with the pore before diffusing away; translocation events, where the molecule threads through the pore with large I and the value of T decreases with increasing voltage; and intercalation events, where the molecule transiently enters the pore but does not translocate with large I and the value of T increases with increasing voltage. CY12‐T1 and CY12‐T2 gave only bumping and translocation events; CY12‐T3 and CY12‐T4 also gave intercalation events, some of which were of very long duration. The results suggest that three uncoiled peptide strands cannot simultaneously thread through the α‐hemolysin pore and that proteins must completely unfold in order to translocate. Copyright © 2010 European Peptide Society and John Wiley & Sons, Ltd.     

New insights on the voltage dependence of the KCa3.1 channel block by internal TBA

We present in this work a structural model of the open IKCa (KCa3.1) channel derived by homology modeling from the MthK channel structure, and used this model to compute the transmembrane potential profile along the channel pore. This analysis showed that the selectivity filter and the region extending from the channel inner cavity to the internal medium should respectively account for 81% and 16% of the transmembrane potential difference. We found however that the voltage dependence of the IKCa block by the quaternary ammonium ion TBA applied internally is compatible with an apparent electrical distance delta of 0.49 +/- 0.02 (n = 6) for negative potentials. To reconcile this observation with the electrostatic potential profile predicted for the channel pore, we modeled the IKCa block by TBA assuming that the voltage dependence of the block is governed by both the difference in potential between the channel cavity and the internal medium, and the potential profile along the selectivity filter region through an effect on the filter ion occupancy states. The resulting model predicts that delta should be voltage dependent, being larger at negative than positive potentials. The model also indicates that raising the internal K+ concentration should decrease the value of delta measured at negative potentials independently of the external K+ concentration, whereas raising the external K+ concentration should minimally affect delta for concentrations >50 mM. All these predictions are born out by our current experimental results. Finally, we found that the substitutions V275C and V275A increased the voltage sensitivity of the TBA block, suggesting that TBA could move further into the pore, thus leading to stronger interactions between TBA and the ions in the selectivity filter. Globally, these results support a model whereby the voltage dependence of the TBA block in IKCa is mainly governed by the voltage dependence of the ion occupancy states of the selectivity filter.     

Conductive properties and gating of channels formed by syringopeptin 25A, a bioactive lipodepsipeptide from Pseudomonas syringae pv. syringae, in planar lipid membranes

Syringopeptin 25A, a pseudomonad lipodepsipeptide, can form ion channels in planar lipid membranes. Pore conductance is around 40 pS in 0.1 M NaCl. Channel opening is strongly voltage dependent and requires a negative potential on the same side of the membrane where the toxin was added. These pores open and close with a lifetime of several seconds. At negative voltages, an additional pore state of around 10 pS and a lifetime of around 30 ms is also present. The voltage dependence of the rates of opening and closing of the stable pores is exponential. This allows estimation of the equivalent charge that is moved across the membrane during the process of opening at about 2.6 elementary charges. When NaCl is present, the pore is roughly 3 times more permeant for anions than for cations. The current voltage characteristic of the pore is nonlinear, i.e., pore conductance is larger at negative than at positive voltages. The maximal conductance of the pore depends on the concentration of the salt present, in a way that varies almost linearly with the conductivity of the solution. From this, an estimate of a minimal pore radius of 0.4 nm was derived.     

The cationically selective state of the mitochondrial outer membrane pore: a study with intact mitochondria and reconstituted mitochondrial porin.

The outer mitochondrial membrane pore at a voltage above 20 to 30 mV can adopt a state of low conductance which may restrict free permeability of mitochondrial substrates. In order to obtain insight into the physiological meaning of this property we took advantage of the fact that the low conductance pore state could be induced by a polyanion in lipid bilayer membranes as well as in intact mitochondria. Upon reconstitution in artificial bilayers the pore in this substate became exclusively cation selective when the polarity of the applied voltage was negative on the cis-side. This behaviour of the pore would explain why induction of the low conductance pore state in intact mitochondria led to a complete inhibition of mitochondrial intermembranous kinases, such as creatine kinase and adenylate kinase, but not of peripheral kinases, for example hexokinase, when utilizing external ATP. The possibility that the inner membrane potential might be transduced to the outer membrane in the contact sites, suggests the existence of cation selective pores in these sites. This aspect may be important in the regulation of peripheral kinases like creatine kinase, nucleoside diphosphate kinase and adenylate kinase which are located behind the outer mitochondrial membrane.     

Elimination and restoration of voltage dependence in the mitochondrial channel,VDAC, by graded modification with succinic anhydride

Summary The major permeability pathways of the outer mitochondrial membrane are the voltage-gated channels called VDAC. It is known that the conductance of these channels decreases as the transmembrane voltage is increased in the positive or negative direction. These channels are known to display a preference for anions over cations of similar size and valence. It was proposed (Doring & Colombini, 1985b) that a set of positive charges lining the channel may be responsible for both voltage dependence and selectivity. A prediction of this proposal is that progressive replacement of the positive charges with negative charges should at first diminish, and then restore, voltage dependence. At the same time, the channel's preference for anions over cations should diminish then reverse. Succinic anhydride was used to perform these experiments as it replaces positively charged amino groups with negatively charged carboxyl groups. When channels, which had been inserted into phospholipid membranes, were treated with moderate amounts of the anhydride, they lost their voltage dependence and preference for anions. With further succinylation, voltage dependence was regenerated while the channels became cation selective. The voltage needed to close one-half of the channels increased in those treatments in which voltage dependence was diminished. As voltage dependence was restored, the voltage needed to close half of the channels decreased. The energy difference between the open and closed state in the absence of an applied field changed little with succinylation, indicating that the procedure did not cause large changes in VDAC's structure but specifically altered those charges responsible for voltage gating and selectivity.     

Localization of a voltage gate in connexin46 gap junction hemichannels.

Cysteine replacement mutagenesis has identified positions in the first transmembrane domain of connexins as contributors to the pore lining of gap junction hemichannels (Zhou et al. 1997. Biophys. J. 72:1946-1953). Oocytes expressing a mutant cx46 with a cysteine in position 35 exhibited a membrane conductance sensitive to the thiol reagent maleimidobutyryl biocytin (MBB). MBB irreversibly reduced the single-channel conductance by 80%. This reactive cysteine was used to probe the localization of a voltage gate that closes cx46 gap junction hemichannels at negative potentials. MBB was applied to the closed channel either from outside (whole cell) or from inside (excised membrane patches). After washout of the thiol reagent the channels were tested at potentials at which the channels open. After extracellular application of MBB to intact oocytes, the membrane conductance was unaffected. In contrast, channels treated with intracellular MBB were blocked. Thus the cysteine in position 35 of cx46 is accessible from inside but not from the outside while the channel is closed. These results suggest that the voltage gate, which may be identical to the "loop gate" (Trexler et al. 1996. Proc. Natl. Acad. Sci. USA. 93:5836-5841), is located extracellular to the 35 position. The voltage gate results in regional closure of the pore rather than closure along the entire pore length.     

Ionic current blockades from DNA and RNA molecules in the alpha-hemolysin nanopore

We characterize the substate structure of current blockades produced when single-stranded polynucleotide molecules were electrophoretically driven into the alpha-hemolysin protein pore. We frequently observe substates where the ionic current is reduced by approximately 50%. Most of these substates can be associated with a molecular configuration where a polymer occupies only the vestibule region of the pore, though a few appear related to a polymer occupying only the transmembrane beta-barrel region of the pore. The duration of the vestibule configuration depends on polymer composition and on which end of the polymer, 3' or 5', subsequently threads into the narrowest constriction and initiates translocation. Below approximately 140 mV a polymer is more likely to escape from the vestibule against the applied voltage gradient, while at higher voltages a polymer is more likely to follow the voltage gradient by threading through the narrowest constriction and translocating through the pore. Increasing the applied voltage also increases the duration of the vestibule configuration. A semiquantitative model of these trends suggests that escape has stronger voltage dependence than threading, and that threading is sensitive to polymer orientation while escape is not. These results emphasize the utility of alpha-hemolysin as a model system to study biologically relevant physical and chemical processes at the single-molecule level.     

Mechanisms of Cs+ blockade in a Ca2+-activated K+ channel from smooth muscle.

Large unitary conductance Ca2+-activated K+ channels from smooth muscle membrane were incorporated into phospholipid planar bilayers, and the blockade induced by internally and externally applied Cs+ was characterized. Internal Cs+ blockade is voltage dependent and can be explained on the basis of a Cs+ binding to a site that senses 54% of the applied voltage, with an apparent dissociation constant, Kd(0), of 70 mM. On the other hand, external Cs+ blocks the channel in micromolar amounts, and the voltage dependence of blockade is a function of Cs+ concentration. The fractional electrical distance can be as large as 1.4 at 10 mM Cs+. This last result suggests that the channel behaves as a multi-ion pore. At large negative voltages the I-V relationships in the presence of external Cs+ show an upturn, indicating relief of Cs+ block. External Cs+ blockade is relieved by increasing the internal K+ concentration, but can be enhanced by increasing the external K+. All the characteristics of external Cs+ block can be explained by a model that incorporates a "knock-on" of Cs+ by K+.     

Water and ion permeability of a claudin model: A computational study

At present, the three‐dimensional structure of the multimeric paracellular claudin pore is unknown. Using extant biophysical data concerning the size of the pore and permeation of water and cations through it, two three‐dimensional models of the pore are constructed in silico. Molecular Dynamics (MD) calculations are then performed to compute water and sodium ion permeation fluxes under the influence of applied hydrostatic pressure. Comparison to experiment is made, under the assumption that the hydrostatic pressure applied in the simulations is equivalent to osmotic pressure induced in experimental measurements of water/ion permeability. One model, in which pore‐lining charged is distributed evenly over a selectivity filter section 10–16 Å in length, is found to be generally consistent with experimental data concerning the dependence of water and ion permeation on channel pore diameter, pore length, and the sign and magnitude of pore lining charge. The molecular coupling mechanism between water and ion flow under conditions where hydrostatic pressure is applied is computationally elucidated. Proteins 2016; 84:305–315. © 2016 Wiley Periodicals, Inc.     

Structural refinement of the hERG1 pore and voltage‐sensing domains with ROSETTA‐membrane and molecular dynamics simulations

The hERG1 gene (Kv11.1) encodes a voltage‐gated potassium channel. Mutations in this gene lead to one form of the Long QT Syndrome (LQTS) in humans. Promiscuous binding of drugs to hERG1 is known to alter the structure/function of the channel leading to an acquired form of the LQTS. Expectably, creation and validation of reliable 3D model of the channel have been a key target in molecular cardiology and pharmacology for the last decade. Although many models were built, they all were limited to pore domain. In this work, a full model of the hERG1 channel is developed which includes all transmembrane segments. We tested a template‐driven de‐novo design with ROSETTA‐membrane modeling using side‐chain placements optimized by subsequent molecular dynamics (MD) simulations. Although backbone templates for the homology modeled parts of the pore and voltage sensors were based on the available structures of KvAP, Kv1.2 and Kv1.2‐Kv2.1 chimera channels, the missing parts are modeled de‐novo. The impact of several alignments on the structure of the S4 helix in the voltage‐sensing domain was also tested. Herein, final models are evaluated for consistency to the reported structural elements discovered mainly on the basis of mutagenesis and electrophysiology. These structural elements include salt bridges and close contacts in the voltage‐sensor domain; and the topology of the extracellular S5‐pore linker compared with that established by toxin foot‐printing and nuclear magnetic resonance studies. Implications of the refined hERG1 model to binding of blockers and channels activators (potent new ligands for channel activations) are discussed. Proteins 2010. © 2010 Wiley‐Liss, Inc.     

Protein electrostriction: a possibility of elastic deformation of the α-hemolysin channel by the applied field

While conformational flexibility of proteins is widely recognized as one of their functionally crucial features and enjoys proper attention for this reason, their elastic properties are rarely discussed. In ion channel studies, where the voltage-induced or ligand-induced conformational transitions, gating, are the leading topic of research, the elastic structural deformation by the applied electric field has never been addressed at all. Here we examine elasticity using a model channel of known crystal structure—Staphylococcus aureus -hemolysin. Working with single channels reconstituted into planar lipid bilayers, we first show that their ionic conductance is asymmetric with voltage even at the highest salt concentration used where the static charges in the channel interior are maximally shielded. Second, choosing 18-crown-6 as a molecular probe whose size is close to the size of the narrowest part of the -hemolysin pore, we analyze the blockage of the channel by the crown/K⁺ complex. Analysis of the blockage within the framework of the Woodhull model in its generalized form demonstrates that the model is able to correctly describe the crown effect only if the parameters of the model are considered to be voltage-dependent. Specifically, one has to include either a voltage-dependent barrier for crown release to the cis side of the channel or voltage-dependent interactions between the binding site and the crown. We suggest that the voltage sensitivity of both the ionic conductance of the channel seen at the highest salt concentration and its blockage by the crown reflects a field-induced deformation of the pore.     

Inhibition of adenine nucleotide transport through the mitochondrial porin by a synthetic polyanion

The effect of a synthetic polyanion of Mr 10,000 (a copolymer of methacrylate, maleate and styrene in a 1:2:3 proportion) was studied on isolated rat liver mitochondria and on mitochondrial porin reconstituted into lipid bilayer membranes. Increasing concentrations of the polyanion inhibited the adenyl kinase located between both mitochondrial membranes in a dose-dependent fashion. Upon addition of the detergent digitonin in increasing concentrations the adenyl kinase activity was fully reversible. In reconstitution experiments with mitochondrial porin the polyanion increased the voltage dependence of the pore in such a way that the pore is switched into the closed state at much smaller voltages than in the absence of the polyanion. The asymmetric addition of the polyanion resulted in an asymmetric shift of the voltage-dependence of the pore. If the voltage is negative at the cis-side (the side of the addition of the polyanion) the pore closed rapidly whereas it was always open for potentials of opposite polarity. The results are discussed on the basis of a modification of the gate properties of the mitochondrial porin by the polyanion and by the assumption that the closed state of the pore is not permeable for nucleotides.     

Intracellular domains interactions and gated motions of IKS potassium channel subunits

Voltage‐gated K⁺ channels co‐assemble with auxiliary β subunits to form macromolecular complexes. In heart, assembly of Kv7.1 pore‐forming subunits with KCNE1 β subunits generates the repolarizing K⁺ current I_KS. However, the detailed nature of their interface remains unknown. Mutations in either Kv7.1 or KCNE1 produce the life‐threatening long or short QT syndromes. Here, we studied the interactions and voltage‐dependent motions of I_KS channel intracellular domains, using fluorescence resonance energy transfer combined with voltage‐clamp recording and in vitro binding of purified proteins. The results indicate that the KCNE1 distal C‐terminus interacts with the coiled‐coil helix C of the Kv7.1 tetramerization domain. This association is important for I_KS channel assembly rules as underscored by Kv7.1 current inhibition produced by a dominant‐negative C‐terminal domain. On channel opening, the C‐termini of Kv7.1 and KCNE1 come close together. Co‐expression of Kv7.1 with the KCNE1 long QT mutant D76N abolished the K⁺ currents and gated motions. Thus, during channel gating KCNE1 is not static. Instead, the C‐termini of both subunits experience molecular motions, which are disrupted by the D76N causing disease mutation.     

Field-dependent effect of crown ether (18-crown-6) on ionic conductance of alpha-hemolysin channels

Closing linear poly(ethylene glycol) (PEG) into a circular "crown" dramatically changes its dynamics in the alpha-hemolysin channel. In the electrically neutral crown ether (C2H4O)6, six ethylene oxide monomers are linked into a circle that gives the molecule ion-complexing capacity and increases its rigidity. As with linear PEG, addition of the crown to the membrane-bathing solution decreases the ionic conductance of the channel and generates additional conductance noise. However, in contrast to linear PEG, both the conductance reduction (reporting on crown partitioning into the channel pore) and the noise (reporting on crown dynamics in the pore) now depend on voltage strongly and nonmonotonically. Within the whole frequency range accessible in channel reconstitution experiments, the noise power spectrum is "white", showing that crown exchange between the channel and the bulk solution is fast. Analyzing these data in the framework of a Markovian two-state model, we are able to characterize the process quantitatively. We show that the lifetime of the crown in the channel reaches its maximum (a few microseconds) at about the same voltage (approximately 100 mV, negative from the side of protein addition) where the crown's reduction of the channel conductance is most pronounced. Our interpretation is that, because of its rigidity, the crown feels an effective steric barrier in the narrowest part of the channel pore. This barrier together with crown-ion complexing and resultant interaction with the applied field leads to behavior usually associated with voltage-dependent binding in the channel pore.     

The K+ channel in the plasma membrane of rye roots has a multiple ion residency pore

The permeation of K⁺ and Na⁺ through the pore of a K⁺ channel from the plasma membrane of rye roots was studied in planar 1-palmitoyl-2-oleoyl phosphatidylethanolamine bilayers. The pore contains at least two ion-binding sites which can be occupied simultaneously. This was indicated by: (i) biphasic relationships with increasing cation concentration of both channel conductance at the zero-current (reversal) potential of the channel (E _rev) and unitary-current at a specified voltage and (ii) a decline in E _rev in the presence of equimolar Na⁺ (cis):K⁺ (trans) as the cation concentration was increased. To determine the spatial characteristics and energy profiles for K⁺ and Na⁺ permeation, unitary-current/ voltage data for the channel were fitted to a three energy-barrier, two ion-binding site (3B2S) model. The model allowed for simultaneous occupancy of binding sites and ionic repulsion within the pore, as well as surface potential effects. Results suggested that energy peaks and energy wells (ion binding sites) were situated asymmetrically within the electrical distance of the pore, the trans energy-well being closer to the center of the pore than its cis counterpart; that the energy profile for K⁺ permeation differed significantly from that of Na⁺ in having a higher cis energy peak and a deeper cis energy well; that cations repelled each other within the pore and that vestibule surface charge was negligible. The model successfully simulated various aspects of K⁺ and Na⁺ permeation including: (i) the complexities in current rectification over a wide range of contrasting ionic conditions; (ii) the biphasic relationships with increasing cation concentration of both channel conductance at E _rev and unitary-current at a specified voltage; (iii) the decline in E _rev in equimolar Na⁺ (cis):K⁺ (trans) as cation concentrations were increased and (iv) the complex relationships between mole fraction and E _rev at total cation concentrations of 100 and 300 mm.We thank Prof. O. Alvarez (Universidad de Chile, Santiago, Chile) for supplying the computer program AJUSTE and Prof. D. Sanders (University of York, UK), Prof. D. Gradmann and Dr. G. Thiel (University of Göttingen, Germany) for stimulating ideas. This work was supported by the Agricultural and Food Research Council.     

Two Separate Interfaces between the Voltage Sensor and Pore Are Required for the Function of Voltage-Dependent K+ Channels

Voltage-dependent K⁺ (Kv) channels gate open in response to the membrane voltage. To further our understanding of how cell membrane voltage regulates the opening of a Kv channel, we have studied the protein interfaces that attach the voltage-sensor domains to the pore. In the crystal structure, three physical interfaces exist. Only two of these consist of amino acids that are co-evolved across the interface between voltage sensor and pore according to statistical coupling analysis of 360 Kv channel sequences. A first co-evolved interface is formed by the S4-S5 linkers (one from each of four voltage sensors), which form a cuff surrounding the S6-lined pore opening at the intracellular surface. The crystal structure and published mutational studies support the hypothesis that the S4-S5 linkers convert voltage-sensor motions directly into gate opening and closing. A second co-evolved interface forms a small contact surface between S1 of the voltage sensor and the pore helix near the extracellular surface. We demonstrate through mutagenesis that this interface is necessary for the function and/or structure of two different Kv channels. This second interface is well positioned to act as a second anchor point between the voltage sensor and the pore, thus allowing efficient transmission of conformational changes to the pore's gate.