Lipids in the structure,folding, and function of the KcsA K+ channel

Lipid molecules surround an ion channel in its native environment of cellular membranes. The importance of the lipid bilayer and the role of lipid protein interactions in ion channel structure and function are not well understood. Here we demonstrate that the bacterial potassium channel KcsA binds a negatively charged lipid molecule. We have defined the potential binding site of the lipid molecule on KcsA by X-ray crystallographic analysis of a complex of KcsA with a monoclonal antibody Fab fragment. We also demonstrate that lipids are required for the in vitro refolding of the KcsA tetramer from the unfolded monomeric state. The correct refolding of the KcsA tetramer requires lipids, but it is not dependent on negatively charged lipids as refolding takes place in the absence of such lipids. We confirm that the presence of negatively charged lipids is required for ion conduction through the KcsA potassium channel, suggesting that the lipid bound to KcsA is important for ion channel function.     

Ion binding to KcsA: implications in ion selectivity and channel gating

Binding of K+ and Na+ to the potassium channel KcsA has been characterized from the stabilization observed in the heat-induced denaturation of the protein as the ion concentration is increased. KcsA thermal denaturation is known to include (i) dissociation of the homotetrameric channel into its constituent subunits and (ii) protein unfolding. The ion concentration-dependent changes in the thermal stability of the protein, evaluated as the Tm value for thermal-induced denaturation of the protein, may suggest the existence of both high- and low-affinity K+ binding sites of KcsA, which lend support to the tenet that channel gating may be governed by K+ concentration-dependent transitions between different affinity states of the channel selectivity filter. We also found that Na+ binds to KcsA with a KD similar to that estimated electrophysiologically from channel blockade. Therefore, our findings on ion binding to KcsA partly account for K+ over Na+ selectivity and Na+ blockade and argue against the strict “snug fit” hypothesis used initially to explain ion selectivity from the X-ray channel structure. Furthermore, the remarkable effects of increasing the ion concentration, K+ in particular, on the Tm of the denaturation process evidence that synergistic effects of the metal-mediated intersubunit interactions at the channel selectivity filter are a major contributor to the stability of the tetrameric protein. This observation substantiates the notion of a role for ions as structural “effectors” of ion channels.     

Contribution of ion binding affinity to ion selectivity and permeation in KcsA, a model potassium channel

Ion permeation and selectivity, key features in ion channel function, are believed to arise from a complex ensemble of energetic and kinetic variables. Here we evaluate the contribution of pore cation binding to ion permeation and selectivity features of KcsA, a model potassium channel. For this, we used E71A and M96V KcsA mutants in which the equilibrium between conductive and nonconductive conformations of the channel is differently shifted. E71A KcsA is a noninactivating channel mutant. Binding of K(+) to this mutant reveals a single set of low-affinity K(+) binding sites, similar to that seen in the binding of K(+) to wild-type KcsA that produces a conductive, low-affinity complex. This seems consistent with the observed K(+) permeation in E71A. Nonetheless, the E71A mutant retains K(+) selectivity, which cannot be explained on the basis of just its low affinity for this ion. At variance, M96V KcsA is a rapidly inactivating mutant that has lost selectivity for K(+) and also conducts Na(+). Here, low-affinity binding and high-affinity binding of both cations are detected, seemingly in agreement with both being permeating species in this mutant channel. In conclusion, binding of the ion to the channel protein seemingly explains certain gating, ion selectivity, and permeation properties. Ion binding stabilizes greatly the channel and, depending upon ion type and concentration, leads to different conformations and ion binding affinities. High-affinity states guarantee binding of specific ions and mediate ion selectivity but are nonconductive. Conversely, low-affinity states would not discriminate well among different ions but allow permeation to occur.     

Structures of Gating Intermediates in a K+ channel

Regulation of ion conduction through the pore of a K⁺ channel takes place through the coordinated action of the activation gate at the bundle crossing of the inner helices and the inactivation gate located at the selectivity filter. The mechanism of allosteric coupling of these gates is of key interest. Here we report new insights into this allosteric coupling mechanism from studies on a W67F mutant of the KcsA channel. W67 is in the pore helix and is highly conserved in K⁺ channels. The KcsA W67F channel shows severely reduced inactivation and an enhanced rate of activation. We use continuous wave EPR spectroscopy to establish that the KcsA W67F channel shows an altered pH dependence of activation. Structural studies on the W67F channel provide the structures of two intermediate states: a pre- open state and a pre-inactivated state of the KcsA channel. These structures highlight key nodes in the allosteric pathway. The structure of the KcsA W67F channel with the activation gate open shows altered ion occupancy at the second ion binding site (S2) in the selectivity filter. This finding in combination with previous studies strongly support a requirement for ion occupancy at the S2 site for the channel to inactivate.     

Structure-guided transformation of charybdotoxin yields an analog that selectively targets Ca(2+)-activated over voltage-gated K(+) channels

We have used a structure-based design strategy to transform the polypeptide toxin charybdotoxin, which blocks several voltage-gated and Ca(2+)-activated K(+) channels, into a selective inhibitor. As a model system, we chose two channels in T-lymphocytes, the voltage-gated channel Kv1.3 and the Ca(2+)-activated channel IKCa1. Homology models of both channels were generated based on the crystal structure of the bacterial channel KcsA. Initial docking of charybdotoxin was undertaken with both models, and the accuracy of these docking configurations was tested by mutant cycle analyses, establishing that charybdotoxin has a similar docking configuration in the external vestibules of IKCa1 and Kv1.3. Comparison of the refined models revealed a unique cluster of negatively charged residues in the turret of Kv1.3, not present in IKCa1. To exploit this difference, three novel charybdotoxin analogs were designed by introducing negatively charged residues in place of charybdotoxin Lys(32), which lies in close proximity to this cluster. These analogs block IKCa1 with approximately 20-fold higher affinity than Kv1.3. The other charybdotoxin-sensitive Kv channels, Kv1.2 and Kv1. 6, contain the negative cluster and are predictably insensitive to the charybdotoxin position 32 analogs, whereas the maxi-K(Ca) channel, hSlo, lacking the cluster, is sensitive to the analogs. This provides strong evidence for topological similarity of the external vestibules of diverse K(+) channels and demonstrates the feasibility of using structure-based strategies to design selective inhibitors for mammalian K(+) channels. The availability of potent and selective inhibitors of IKCa1 will help to elucidate the role of this channel in T-lymphocytes during the immune response as well as in erythrocytes and colonic epithelia.     

Preparation and properties of asymmetric large unilamellar vesicles: interleaflet coupling in asymmetric vesicles is dependent on temperature but not curvature

Using both Brownian and molecular dynamics, we replicate many of the salient features of Kv1.2, including the current-voltage-concentration profiles and the binding affinity and binding mechanisms of charybdotoxin, a scorpion venom. We also elucidate how structural differences in the inner vestibule can give rise to significant differences in its permeation characteristics. Current-voltage-concentration profiles are constructed using Brownian dynamics simulations, based on the crystal structure 2A79. The results are compatible with experimental data, showing similar conductance, rectification, and saturation with current. Unlike KcsA, for example, the inner pore of Kv1.2 is mainly hydrophobic and neutral, and to explore the consequences of this, we investigate the effect of mutating neutral proline residues at the mouth of the inner vestibule to charged aspartate residues. We find an increased conductance, less inward rectification, and quicker saturation of the current-voltage profile. Our simulations use modifications to our Brownian dynamics program that extend the range of channels that can be usefully modeled. Using molecular dynamics, we investigate the binding of the charybdotoxin scorpion venom to the outer vestibule of the channel. A potential of mean force is derived using umbrella sampling, giving a dissociation constant within a factor of ∼2 to experimentally derived constants. The residues involved in the toxin binding are in agreement with experimental mutagenesis studies. We thus show that the experimental observations on the voltage-gated channel, including the toxin-channel interaction, can reliably be replicated by using the two widely used computational tools.     

Special Interaction of Anionic Phosphatidic Acid Promotes High Secondary Structure in Tetrameric Potassium Channel

Anionic phosphatidic acid (PA) has been shown to stabilize and bind stronger than phosphatidylglycerol via electrostatic and hydrogen bond interaction with the positively charged residues of potassium channel KcsA. However, the effects of these lipids on KcsA folding or secondary structure are not clear. In this study, the secondary structure analyses of KcsA potassium channel was carried out using circular dichroism spectroscopy. It was found that PA interaction leads to increases in α-helical and β-sheet content of KcsA protein. In PA, KcsA α-helical structure was further stabilized by classical membrane-active cosolvent trifluoroethanol followed by reduction in the β-sheet content indicating cooperative transformation from the β-sheet to an α-helical structure. The data further uncover the role of anionic PA in KcsA folding and provide mechanism by which strong hydrogen bonds/electrostatic interaction among PA headgroup and basic residues on lipid binding domains may induce high helical structure thereby altering the protein folding and increasing the stability of tetrameric assembly.     

N-type inactivation of the potassium channel KcsA by the Shaker B "ball" peptide: mapping the inactivating peptide-binding epitope

The effects of the inactivating peptide from the eukaryotic Shaker BK(+) channel (the ShB peptide) on the prokaryotic KcsA channel have been studied using patch clamp methods. The data show that the peptide induces rapid, N-type inactivation in KcsA through a process that includes functional uncoupling of channel gating. We have also employed saturation transfer difference (STD) NMR methods to map the molecular interactions between the inactivating peptide and its channel target. The results indicate that binding of the ShB peptide to KcsA involves the ortho and meta protons of Tyr(8), which exhibit the strongest STD effects; the C4H in the imidazole ring of His(16); the methyl protons of Val(4), Leu(7), and Leu(10) and the side chain amine protons of one, if not both, the Lys(18) and Lys(19) residues. When a noninactivating ShB-L7E mutant is used in the studies, binding to KcsA is still observed but involves different amino acids. Thus, the strongest STD effects are now seen on the methyl protons of Val(4) and Leu(10), whereas His(16) seems similarly affected as before. Conversely, STD effects on Tyr(8) are strongly diminished, and those on Lys(18) and/or Lys(19) are abolished. Additionally, Fourier transform infrared spectroscopy of KcsA in presence of (13)C-labeled peptide derivatives suggests that the ShB peptide, but not the ShB-L7E mutant, adopts a beta-hairpin structure when bound to the KcsA channel. Indeed, docking such a beta-hairpin structure into an open pore model for K(+) channels to simulate the inactivating peptide/channel complex predicts interactions well in agreement with the experimental observations.     

Hierarchical approach to predicting permeation in ion channels

A hierarchical computational strategy combining molecular modeling, electrostatics calculations, molecular dynamics, and Brownian dynamics simulations is developed and implemented to compute electrophysiologically measurable properties of the KcsA potassium channel. Models for a series of channels with different pore sizes are developed from the known x-ray structure, using insights into the gating conformational changes as suggested by a variety of published experiments. Information on the pH dependence of the channel gating is incorporated into the calculation of potential profiles for K(+) ions inside the channel, which are then combined with K(+) ion mobilities inside the channel, as computed by molecular dynamics simulations, to provide inputs into Brownian dynamics simulations for computing ion fluxes. The open model structure has a conductance of approximately 110 pS under symmetric 250 mM K(+) conditions, in reasonable agreement with experiments for the largest conducting substate. The dimensions of this channel are consistent with electrophysiologically determined size dependence of quaternary ammonium ion blocking from the intracellular end of this channel as well as with direct structural evidence that tetrabutylammonium ions can enter into the interior cavity of the channel. Realistic values of Ussing flux ratio exponents, distribution of ions within the channel, and shapes of the current-voltage and current-concentration curves are obtained. The Brownian dynamics calculations suggest passage of ions through the selectivity filter proceeds by a "knock-off" mechanism involving three ions, as has been previously inferred from functional and structural studies of barium ion blocking. These results suggest that the present calculations capture the essential nature of K(+) ion permeation in the KcsA channel and provide a proof-of-concept for the integrated microscopic/mesoscopic multitiered approach for predicting ion channel function from structure, which can be applied to other channel structures.     

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

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

Binding of kappa-conotoxin PVIIA to Shaker K+ channels reveals different K+ and Rb+ occupancies within the ion channel pore

The x-ray structure of the KcsA channel at different [K(+)] and [Rb(+)] provided insight into how K(+) channels might achieve high selectivity and high K(+) transit rates and showed marked differences between the occupancies of the two ions within the ion channel pore. In this study, the binding of kappa-conotoxin PVIIA (kappa-PVIIA) to Shaker K(+) channel in the presence of K(+) and Rb(+) was investigated. It is demonstrated that the complex results obtained were largely rationalized by differences in selectivity filter occupancy of this 6TM channels as predicted from the structural work on KcsA. kappa-PVIIA inhibition of the Shaker K(+) channel differs in the closed and open state. When K(+) is the only permeant ion, increasing extracellular [K(+)] decreases kappa-PVIIA affinity for closed channels by decreasing the "on" binding rate, but has no effect on the block of open channels, which is influenced only by the intracellular [K(+)]. In contrast, extracellular [Rb(+)] affects both closed- and open-channel binding. As extracellular [Rb(+)] increases, (a) binding to the closed channel is slightly destabilized and acquires faster kinetics, and (b) open channel block is also destabilized and the lowest block seems to occur when the pore is likely filled only by Rb(+). These results suggest that the nature of the permeant ions determines both the occupancy and the location of the pore site from which they interact with kappa-PVIIA binding. Thus, our results suggest that the permeant ion(s) within a channel pore can determine its functional and pharmacological properties.     

Design and characterization of a constitutively open KcsA

The molecular nature of the structure responsible for proton sensitivity in KcsA has been identified as a charge cluster that surrounds the inner helical bundle gate. Here, we show that this proton sensor can be modified to engineer a constitutively open form of KcsA, amenable to functional, spectroscopic and structural analyses. By combining charge neutralizations for all acidic and basic residues in the cluster at positions 25, 117-122 and 124 (but not E118), a mutant KcsA is generated that displays constitutively open channel activity up to pH 9. The structure of this mutant revealed that full opening appears to be inhibited by lattice forces since the activation gate seems to be only on the early stages of opening.     

Structural basis of the KcsA K(+) channel and agitoxin2 pore-blocking toxin interaction by using the transferred cross-saturation method

We have determined the binding site on agitoxin2 (AgTx2) to the KcsA K(+) channel by a transferred cross-saturation (TCS) experiment. The residues significantly affected in the TCS experiments formed a contiguous surface on AgTx2, and substitutions of the surface residues decreased the binding affinity to the KcsA K(+) channel. Based on properties of the AgTx2 binding site with the KcsA K(+) channel, we present a surface motif that is observed in pore-blocking toxins affecting the K(+) channel. Furthermore, we also explain the structural basis of the specificity of the K(+) channel to the toxins. The TCS method utilized here is applicable not only for the channels, which are complexed with other inhibitors, but also with a variety of regulatory molecules, and provides important information about their interface in solution.     

Structural differences of bacterial and mammalian K+ channels

Using a peptide toxin, kaliotoxin (KTX), we gained new insight into the topology of the pore region of a voltage-gated potassium channel, mKv1.1. In order to find new interactions between mKv1.1 and KTX, we investigated the pH dependence of KTX block which was stronger at pH(o) 6.2 compared with pH(o) 7.4. Using site-directed mutagenesis on the channel and the toxin, we found that protonation of His(34) in KTX caused the pH(o) dependence of KTX block. Glu(350) and Glu(353) in mKv1.1, which interact with His(34) in KTX, were calculated to be 4 and 7 A away from His(34)/KTX, respectively. Docking of KTX into a homology model of mKv1.1 based on the KcsA crystal structure using this and other known interactions as constraints showed structural differences between mKv1.1 and KcsA within the turret (amino acids 348-357). To satisfy our data, we would have to modify the KcsA crystal structure for the mKv1.1 channel orienting Glu(350) 7 A and Glu(353) 4 A more toward the center of the pore compared with KcsA. This would place Glu(350) 15 A and Glu(353) 11 A away from the center of the pore instead of the distances for the equivalent KcsA residues with 22 A for Gly(53) and 15 A for Gly(56), respectively. Bacterial and mammalian potassium channels may have structural differences regarding the turret of the outer pore vestibule. This topological difference between both channel types may have substantial influence on structure-guided development of new drugs for mammalian potassium channels by rational drug design.     

Interaction of agitoxin2, charybdotoxin,and iberiotoxin with potassium channels: selectivity between voltage-gated and Maxi-K channels

To gain insight into the molecular determinants that define the specificity of interaction of pore-blocking peptides, such as agitoxin 2 (AgTX2), charybdotoxin (ChTX), and iberiotoxin (IbTX) with the Shaker-type voltage-gated potassium channel Kv1.3, or the large-conductance Ca(2+)-activated K(+) (Maxi-K) channel, homology models of these channels were generated based on the crystal structure of the bacterial, KcsA, potassium channel. Peptide-channel complexes were analyzed to evaluate the predicted interaction interfaces between the peptides and the channels' outer vestibules. The docking model, for either AgTX2 or ChTX with the Kv1.3 channel, predicts a novel hydrogen bonding interaction between the Asn30 side-chain of the peptide and the Asp381 side-chain of the channel. This interaction is consistent with the >500-fold decreased potency of both AgTX2 and ChTX mutants at position 30 for the Shaker channel [(Ranganathan et al., Neuron 1996;16:131-139); (Goldstein et al., Neuron 1994;12:1377-1388)]. This hydrogen bonding interaction also suggests that Gly30 in IbTX may be the critical determinant for its lack of activity against Shaker Kv channels. The model of the Maxi-K channel reveals a narrower and more structurally restrained outer vestibule in which the aromatic residues Phe266 and Tyr294 may stabilize binding of IbTX and ChTX by pi-pi stacking with the aromatic residues Trp14 and Tyr36 of the peptides. This study also suggests that the extra net negative charge of IbTX is not related to the selectivity of this peptide for the Maxi-K channel.     

Comparative study of the energetics of ion permeation in Kv1.2 and KcsA potassium channels

Biological ion channels rely on a multi-ion transport mechanism for fast yet selective permeation of ions. The crystal structure of the KcsA potassium channel provided the first microscopic picture of this process. A similar mechanism is assumed to operate in all potassium channels, but the validity of this assumption has not been well investigated. Here, we examine the energetics of ion permeation in Shaker Kv1.2 and KcsA channels, which exemplify the six-transmembrane voltage-gated and two-transmembrane inward-rectifier channels. We study the feasibility of binding a third ion to the filter and the concerted motion of ions in the channel by constructing the potential of mean force for K⁺ ions in various configurations. For both channels, we find that a pair of K⁺ ions can move almost freely within the filter, but a relatively large free-energy barrier hinders the K⁺ ion from stepping outside the filter. We discuss the effect of the CMAP dihedral energy correction that was recently incorporated into the CHARMM force field on ion permeation dynamics.     

A KcsA/MloK1 Chimeric Ion Channel Has Lipid-dependent Ligand-binding Energetics

Cyclic nucleotide-modulated ion channels play crucial roles in signal transduction in eukaryotes. The molecular mechanism by which ligand binding leads to channel opening remains poorly understood, due in part to the lack of a robust method for preparing sufficient amounts of purified, stable protein required for structural and biochemical characterization. To overcome this limitation, we designed a stable, highly expressed chimeric ion channel consisting of the transmembrane domains of the well characterized potassium channel KcsA and the cyclic nucleotide-binding domains of the prokaryotic cyclic nucleotide-modulated channel MloK1. This chimera demonstrates KcsA-like pH-sensitive activity which is modulated by cAMP, reminiscent of the dual modulation in hyperpolarization-activated and cyclic nucleotide-gated channels that display voltage-dependent activity that is also modulated by cAMP. Using this chimeric construct, we were able to measure for the first time the binding thermodynamics of cAMP to an intact cyclic nucleotide-modulated ion channel using isothermal titration calorimetry. The energetics of ligand binding to channels reconstituted in lipid bilayers are substantially different from those observed in detergent micelles, suggesting that the conformation of the chimera''s transmembrane domain is sensitive to its (lipid or lipid-mimetic) environment and that ligand binding induces conformational changes in the transmembrane domain. Nevertheless, because cAMP on its own does not activate these chimeric channels, cAMP binding likely has a smaller energetic contribution to gating than proton binding suggesting that there is only a small difference in cAMP binding energy between the open and closed states of the channel.     

The occupancy of ions in the K+ selectivity filter: charge balance and coupling of ion binding to a protein conformational change underlie high conduction rates

Potassium ions diffuse across the cell membrane in a single file through the narrow selectivity filter of potassium channels. The crystal structure of the KcsA K+ channel revealed the chemical structure of the selectivity filter, which contains four binding sites for K+. In this study, we used Tl+ in place of K+ to address the question of how many ions bind within the filter at a given time, i.e. what is the absolute ion occupancy? By refining the Tl+ structure against data to 1.9A resolution with an anomalous signal, we determined the absolute occupancy of Tl+. Then, by comparing the electron density of Tl+ with that of K+, Rb+ and Cs+, we estimated the absolute occupancy of these three ions. We further analyzed how the ion occupancy affects the conformation of the selectivity filter by analyzing the structure of KcsA at different concentrations of Tl+. Our results indicate that the average occupancy for each site in the selectivity filter is about 0.63 for Tl+ and 0.53 for K+. For K+, Rb+ and Cs+, the total number of ions contained within four sites in the selectivity filter is about two. At low concentrations of permeant ion, the number of ions drops to one in association with a conformational change in the selectivity filter. We conclude that electrostatic balance and coupling of ion binding to a protein conformational change underlie high conduction rates in the setting of high selectivity.