Potassium and sodium binding to the outer mouth of the K+ channel.

Molecular dynamics simulations of the K+ channel from Streptomyces lividans (KcsA channel) were performed in a membrane-mimetic environment with Na+ and K+ in different initial locations. The structure of the channel remained stable and well preserved for simulations lasting up to 1.5 ns. Salt bridges between Asp80 and Arg89 of neighboring subunits, not detected in the X-ray structure, enhanced the stability of the tetrameric structure. Na+ or K+ ions located in the channel vestibule lost part of their hydration shell and diffused into the channel inner pore in less than a few hundred picoseconds. This powerful catalytic action was caused by strong electrostatic interactions with Asp80 and Glu71. The hydration state of the metal ions turned out to depend significantly on the conformational flexibility of the channel. Furthermore, Na+ entered the channel inner pore bound to more water molecules than K+. The different hydration state of the two ions may be a determinant factor in the ion selectivity of the channel.     

Shaker potassium channel gating. II: Transitions in the activation pathway

Voltage-dependent gating behavior of Shaker potassium channels without N-type inactivation (ShB delta 6-46) expressed in Xenopus oocytes was studied. The voltage dependence of the steady-state open probability indicated that the activation process involves the movement of the equivalent of 12-16 electronic charges across the membrane. The sigmoidal kinetics of the activation process, which is maintained at depolarized voltages up to at least +100 mV indicate the presence of at least five sequential conformational changes before opening. The voltage dependence of the gating charge movement suggested that each elementary transition involves 3.5 electronic charges. The voltage dependence of the forward opening rate, as estimated by the single- channel first latency distribution, the final phase of the macroscopic ionic current activation, the ionic current reactivation and the ON gating current time course, showed movement of the equivalent of 0.3 to 0.5 electronic charges were associated with a large number of the activation transitions. The equivalent charge movement of 1.1 electronic charges was associated with the closing conformational change. The results were generally consistent with models involving a number of independent and identical transitions with a major exception that the first closing transition is slower than expected as indicated by tail current and OFF gating charge measurements.     

Probing the outer mouth structure of the HERG channel with peptide toxin footprinting and molecular modeling

Previous studies have shown that the unusually long S5-P linker lining human ether a-go-go related gene's (hERG's) outer vestibule is critical for its channel function: point mutations at high-impact positions here can interfere with the inactivation process and, in many cases, also reduce the pore's K+ selectivity. Because no data are available on the equivalent region in the available K channel crystal structures to allow for homology modeling, we used alternative approaches to model its three-dimensional structure. The first part of this article describes mutant cycle analysis used to identify residues on hERG's outer vestibule that interact with specific residues on the interaction surface of BeKm-1, a peptide toxin with known NMR structure and a high binding affinity to hERG. The second part describes molecular modeling of hERG's pore domain. The transmembrane region was modeled after the crystal structure of KvAP pore domain. The S5-P linker was docked to the transmembrane region based on data from previous NMR and mutagenesis experiments, as well as a set of modeling criteria. The models were further restrained by contact points between hERG's outer vestibule and the bound BeKm-1 toxin molecule deduced from the mutant cycle analysis. Based on these analyses, we propose a working model for the open conformation of the outer vestibule of the hERG channel, in which the S5-P linkers interact with the pore loops to influence ion flux through the pore.     

Unique interaction of scorpion toxins with the hERG channel

ERG potassium channels specify one component of the delayed rectifier in the heart and are likely to play an important functional role in other excitable cells. Compared to other K+ channels, the human ERG (hERG) channel possesses an unusually long S5-P linker that presumably forms an alpha-helix important for channel function. hERG-specific toxins bind to the outer mouth of the hERG channel. Channel residues in the middle of the S5-P linker and at the pore entrance are critical for toxin binding. One of these scorpion toxins is BeKm-1. Residues critical for BeKm-1 binding to the hERG channel are located in the alpha-helix and the following loop, whereas the "traditional" interaction surface of other short scorpion toxins is formed by residues on the beta-sheet. This unique localization of BeKm-1's interaction surface and its specific action on the hERG channel suggest a unique outer mouth structure of the hERG channel. We used the mutant cycle analysis approach to define contacts in the toxin-channel complex. This information provides critical constraints and is important for molecular modeling of the hERG pore structure.     

A negatively charged residue in the outer mouth of rat sodium channel determines the gating kinetics of the channel

Previous studies using combined techniques of site-directed mutagenesis and electrophysiology of voltage-gated Na(+) channels have demonstrated that there are significant overlaps in the regions that are important for the two fundamental properties of the channels, namely gating and permeation. We have previously shown that a pore-lining residue, W402 in S5-S6 region (P loop) in domain I of the micro1 skeletal muscle Na(+) channel, was important in the gating of the channel. Here, we determined the role of an adjacent pore-lining negatively charged residue (E403) in channel gating. Charge neutralization or substitution with positively charged side chain at this position resulted in a marked delay in the rate of recovery from slow inactivation. Indeed, the fast inactivation process appeared intact. Restoration of the negatively charged side chain with a sulfhydryl modifier, MTS-ethylsulfonate, resulted in a reactivation profile from a slow-inactivated state, which was indistinguishable from that of the wild-type channels. We propose an additional functional role for the negatively charged residue. Assuming no major changes in the pore structure induced by the mutations, the negatively charged residue E403 may work in concert with other pore regions during recovery from slow inactivation of the channel. Our data represent the first report indicating the role of negative charge in the slow inactivation of the voltage-gated Na(+) channel.     

Tetraethylammonium binding to the outer mouth of the KcsA potassium channel: implications for ion permeation

Extracellular tetraethylammonium (TEA+) inhibits the current carried out by K+ ions in potassium channels. Structural models of wild-type (WT) and Y82C KcsA K+ channel/TEA+ complexes are here built using docking procedures, electrostatics calculations and molecular dynamics simulations. The calculations are based on the structure determined by Doyle et al. (11) Our calculations suggest that in WT, the TEA+ cation turns binds at the outer mouth of the selectivity filter, stabilized by electrostatic and hydrophobic interactions with the four Tyr82 side chains. Replacement of Tyr82 with Cys causes a decrease of the affinity of the cation for the channel, consistently with the available site-directed mutagenesis data (16). An MD simulation in which K+ replaces TEA+ provides evidence that TEA+ binding site can accommodate a potassium ion, in agreement with the high-resolution structure recently reported by Zhou et al. (20)     

Shaker potassium channel gating. I: Transitions near the open state

Kinetics of single voltage-dependent Shaker potassium channels expressed in Xenopus oocytes were studied in the absence of fast N-type inactivation. Comparison of the single-channel first latency distribution and the time course of the ensemble average current showed that the activation time course and its voltage dependence are largely determined by the transitions before first opening. The open dwell time data are consistent with a single kinetically distinguishable open state. Once the channel opens, it can enter at least two closed states which are not traversed frequently during the activation process. The rate constants for the transitions among these closed states and the open state are nearly voltage-independent at depolarized voltages (> - 30 mV). During the deactivation process at more negative voltages, the channel can close directly to a closed state in the activation pathway in a voltage-dependent fashion.     

Conduction properties of the cloned Shaker K+ channel.

The conduction properties of the cloned Shaker K+ channel were studied using electrophysiological techniques. Single channel conductance increases in a sublinear manner with symmetric increases in K+ activity, reaching saturation by 0.6 M K+. The Shaker K+ channel is highly selective among monovalent cations; under bi-ionic conditions, its selectivity sequence is K+ > Rb+ > NH+4 > Cs+ > Na+, whereas, by relative conductance in symmetric solutions, it is K+ > NH+4 > Rb+ > Cs+. In Cs+ solutions, single channel currents were too small to be measured directly, so nonstationary fluctuation analysis was used to determine the unitary Cs+ conductance. The single channel conductance displays an anomalous molefraction effect in symmetric mixtures of K+ and NH+4, suggesting that the conducting pore is occupied by multiple ions simultaneously.     

Effects of external stimuli on the pacemaker function of the sinoatrial node in sodium channel gene mutations models

Loss of function and gain of function mutations of the sodium channel were investigated using an intact two-dimensional rabbit sinoatrial node (SAN) and atrial cell model. The effects of three external stimuli (acetylcholine secretion by the vagal nerve, acid-base concentration, and tissue temperature) on cardiac pacemaker function and conduction were studied. Our results show that these two groups of mutations have different effects on pacemaker function and conduction. Furthermore, we found that the negative effects of these mutations could be altered by external stimuli. The bradycardic effects of mutations were magnified by an increase in acetylcholine level. Changes in acid-base concentration and tissue temperature increased the ability of the SAN to recover its pacemaker function. The results of this study increase our understanding of sodium channel disorders, and help to advance research on the treatment of these conditions.     

Characterization and function of the mitochondrial outer membrane peptide-sensitive channel

The PSC (peptide-sensitive Channel), a cationic channel of large conductance, has been characterized in yeast and mammalian mitochondria by three different methods, tip-dip, patch clamp of giant liposomes, and planar bilayers. The yeast and mammalian PSC share the common property to be blocked by basic peptides such as pCyt OX IV (1–12)Y which contains the first 12 residues of the presequence of cytochromec oxidase subunit IV. The electrophysiological data are consistent with a translocation of the peptide through the pore. Analysis of the frequency of observation of the PSC in different fractions indicates that the channel is located in the outer mitochondrial membrane. Uptake measurements of iodinated peptides by intact mitochondria from a porin-less mutant show that the peptides are translocated through the outer membrane, presumably at the level of PSC. Among the peptides active on PSC, several, such as pCyt OX IV (1–22) and the reduced form of the mast cell degranulating peptide, induce an alteration of the voltage dependence or of the inactivation rate subsisting after washing and which is eliminated only by proteolysis of the interacting peptide. These irreversible effects may account for the variability of the properties of the PSC which would interact with cytosolic or intermembrane cations, peptides, or proteins, thus modulating the channel permeability. Finally, several lines of evidence suggest the participation of the PSC in protein translocation and some interaction with the general insertion pore of the outer membrane translocation machinery.     

Gating at the mouth of the acetylcholine receptor channel: energetic consequences of mutations in the alphaM2-cap

Gating of nicotinic acetylcholine receptors from a C(losed) to an O(pen) conformation is the initial event in the postsynaptic signaling cascade at the vertebrate nerve-muscle junction. Studies of receptor structure and function show that many residues in this large, five-subunit membrane protein contribute to the energy difference between C and O. Of special interest are amino acids located at the two transmitter binding sites and in the narrow region of the channel, where C<-->O gating motions generate a low<-->high change in the affinity for agonists and in the ionic conductance, respectively. We have measured the energy changes and relative timing of gating movements for residues that lie between these two locations, in the C-terminus of the pore-lining M2 helix of the alpha subunit ('alphaM2-cap'). This region contains a binding site for non-competitive inhibitors and a charged ring that influences the conductance of the open pore. alphaM2-cap mutations have large effects on gating but much smaller effects on agonist binding, channel conductance, channel block and desensitization. Three alphaM2-cap residues (alphaI260, alphaP265 and alphaS268) appear to move at the outset of channel-opening, about at the same time as those at the transmitter binding site. The results suggest that the alphaM2-cap changes its secondary structure to link gating motions in the extracellular domain with those in the channel that regulate ionic conductance.     

Ligand-activated ion channels may share common gating mechanisms with the Shaker potassium channel.

This paper proposes a detailed gating mechanism for the N-methyl-D-aspartate (NMDA) channel. In the NMDAR1 subunit, the signal of agonist binding may be carried from Y456 to W590 through an electron transport chain, including W480 which could be the glycine modulatory site. The channel's opening may arise from repulsion between negatively charged W590s, analogous to W435s of the Shaker K+ channel. The cyclic nucleotide-gated channels may be activated by a similar mechanism, but the opening of nicotinic acetylcholine receptor (nAChR) channels is likely to be initiated by the formation of tyrosine radicals. The role of disulfide-bonded cysteines in the redox modulation can also be explained.     

Closing in on the resting state of the Shaker K(+) channel

Membrane depolarization causes voltage-gated ion channels to transition from a resting/closed conformation to an activated/open conformation. We used voltage-clamp fluorometry to measure protein motion at specific regions of the Shaker Kv channel. This enabled us to construct new structural models of the resting/closed and activated/open states based on the Kv1.2 crystal structure using the Rosetta-Membrane method and molecular dynamics simulations. Our models account for the measured gating charge displacement and suggest a molecular mechanism of activation in which the primary voltage sensors, S4s, rotate by approximately 180 degrees as they move "outward" by 6-8 A. A subsequent tilting motion of the S4s and the pore domain helices, S5s, of all four subunits induces a concerted movement of the channel's S4-S5 linkers and S6 helices, allowing ion conduction. Our models are compatible with a wide body of data and resolve apparent contradictions that previously led to several distinct models of voltage sensing.     

Drug block of the hERG potassium channel: insight from modeling

Many commonly used, structurally diverse, drugs block the human ether-a-go-go-related gene (hERG) K(+) channel to cause acquired long QT syndrome, which can lead to sudden death via lethal cardiac arrhythmias. This undesirable side effect is a major hurdle in the development of safe drugs. To gain insight about the structure of hERG and the nature of drug block we have produced structural models of the channel pore domain, into each of which we have docked a set of 20 hERG blockers. In the absence of an experimentally determined three-dimensional structure of hERG, each of the models was validated against site-directed mutagenesis data. First, hERG models were produced of the open and closed channel states, based on homology with the prokaryotic K(+) channel crystal structures. The modeled complexes were in partial agreement with the mutagenesis data. To improve agreement with mutagenesis data, a KcsA-based model was refined by rotating the four copies of the S6 transmembrane helix half a residue position toward the C-terminus, so as to place all residues known to be involved in drug binding in positions lining the central cavity. This model produces complexes that are consistent with mutagenesis data for smaller, but not larger, ligands. Larger ligands could be accommodated following refinement of this model by enlarging the cavity using the inherent flexibility about the glycine hinge (Gly648) in S6, to produce results consistent with the experimental data for the majority of ligands tested.     

昆虫击倒抗性基因突变对钠通道功能的影响

该文综述了昆虫钠通道基因的表达与功能特性、击倒抗性突变的功能和这些突变对钠通道门控的影响,以及钠通道基因突变与抗性表现型之间的因果关系;还讨论了这些突变增强击倒抗性的分子机理。     

Probing the outer vestibule of a sodium channel voltage sensor.

The second and third basic residues of the S4 segment of domain 4 (D4:R2 and D4:R3) of the human skeletal muscle Na+ channel are known to be translocated from a cytoplasmic to an extracellular position during depolarization. Accessibilities of individual S4 residues were assayed by alteration of inactivation kinetics during modification of cysteine mutants by hydrophilic methanethiosulfonate reagents. The voltage dependences of the reaction rates are identical for extracellular application of cationic methanethiosulfonate-ethyltrimethylammonium (MTSET) and anionic methanethiosulfonate-ethylsulfonate (MTSES), suggesting that D4:R3C is situated outside the membrane electric field at depolarized voltages. The absolute rate of R3C modification is 281-fold greater for MTSET than for MTSES, however, suggesting that at depolarized voltages this S4 thiol resides in a negatively charged hydrophilic crevice. The two hydrophobic residues between D4:R2C and D4:R3C in the primary sequence (L1452 and A1453) are not externally exposed at any voltage. An alpha-helical representation of D4/S4 shows that the basic residues D4:R2 and D4:R3 are on the face opposite that of L1452 and A1453. We propose that in the depolarized conformation, the hydrophobic face of this portion of D4/S4 remains in contact with a hydrophobic region of the extracellular vestibule of the S4 channel.     

Electrostatic mutations in iberiotoxin as a unique tool for probing the electrostatic structure of the maxi-K channel outer vestibule

Iberiotoxin (IbTX or alpha-KTx 1.3), a selective, high-affinity blocker of the large-conductance, calcium-activated (maxi-K) channel, exhibits a unique, asymmetric distribution of charge. To test how these charges control kinetics of IbTX binding, we generated five mutants at two positions, K27 and R34, that are highly conserved among other isotoxins. The dissociation and association rate constants, koff and kon, were determined from toxin-blocked and -unblocked durations of single maxi-K channels incorporated into planar lipid bilayers. Equilibrium dissociation constant (Kd) values were calculated from koff/kon. The IbTX mutants K27N, K27Q, and R34N caused large increases in Kd values compared to wild-type, suggesting that the IbTX interaction surface encompasses these residues. A well-established pore-blocking mechanism for IbTX predicts a voltage dependence of toxin-blocked times following occupancy of a potassium binding site in the channel pore. Time constants for block by K27R were approximately 5-fold slower at -20 mV versus +40 mV, while neutralization of K27 relieved the voltage dependence of block. This suggests that K27 in IbTX interacts with a potassium binding site in the pore. Neutralized mutants of K27 and R34, with zero net charge, displayed toxin association rate constants approximately 10-fold slower than wild-type. Association rates for R34N diminished approximately 19-fold when external potassium was increased from 30 to 300 mM. These findings suggest that simple net charge and diffusional processes do not control ingress of IbTX into the channel vestibule.