Molecular basis of charge movement in voltage-gated sodium channels

Nonequilibrium gating and voltage dependence of the ClC-0 Cl- channel

The gating of ClC-0, the voltage-dependent Cl- channel from Torpedo electric organ, is strongly influenced by Cl- ions in the external solution. Raising external Cl- over the range 1-600 mM favors the fast-gating open state and disfavors the slow-gating inactivated state. Analysis of purified single ClC-0 channels reconstituted into planar lipid bilayers was used to identify the role of Cl- ions in the channel's fast voltage-dependent gating process. External, but not internal, Cl- had a major effect on the channel's opening rate constant. The closing rate was more sensitive to internal Cl- than to external Cl-. Both opening and closing rates varied with voltage. A model was derived that postulates (a) that in the channel's closed state, Cl- is accessible to a site located at the outer end of the conduction pore, where it binds in a voltage-independent fashion, (b) that this closed conformation can open, whether liganded by Cl- or not, in a weakly voltage-dependent fashion, (c) that the Cl(-)-liganded closed channel undergoes a conformational change to a different closed state, such that concomitant with this change, Cl- ion moves inward, conferring voltage-dependence to this step, and (d) that this new Cl(-)-liganded closed state opens with a very high rate. According to this picture, Cl- movement within the pre-open channel is the major source of voltage dependence, and charge movement intrinsic to the channel protein contributes very little to voltage-dependent gating of ClC-0. Moreover, since the Cl- activation site is probably located in the ion conduction pathway, the fast gating of ClC-0 is necessarily coupled to ion conduction, a nonequilibrium process.

Voltage-sensing residues in the S2 and S4 segments of the Shaker K+ channel

The activation of Shaker K+ channels is steeply voltage dependent. To determine whether conserved charged amino acids in putative transmembrane segments S2, S3, and S4 contribute to the gating charge of the channel, the total gating charge movement per channel was measured in channels containing neutralization mutations. Of eight residues tested, four contributed significantly to the gating charge: E293, an acidic residue in S2, and R365, R368, and R371, three basic residues in the S4 segment. The results indicate that these residues are a major component of the voltage sensor. Furthermore, the S4 segment is not solely responsible for gating charge movement in Shaker K+ channels.

Dynamic rearrangement of the outer mouth of a K+ channel during gating

With prolonged stimulation, voltage-activated K+ channels close by a gating process called inactivation. This inactivation gating can occur by two distinct molecular mechanisms: N-type, in which a tethered particle blocks the intracellular mouth of the pore, and C-type, which involves a closure of the external mouth. The functional motion involved in C-type inactivation was studied by introducing cysteine residues at the outer mouth of Shaker K+ channels through mutagenesis, and by measuring state-dependent changes in accessibility to chemical modification. Modification of three adjacent residues in the outer mouth was 130-10,000-fold faster in the C-type inactivated state than in the closed state. At one position, state-dependent bridging or crosslinking between subunits was also possible. These results give a consistent picture in which C-type inactivation promotes a local rearrangement and constriction of the channel at the outer mouth.

Interactions between a pore-blocking peptide and the voltage sensor of the sodium channel: an electrostatic approach to channel geometry

Few experimental data illuminate the relationship between the molecular structures that mediate ion conduction through voltage-dependent ion channels and the structures responsible for sensing transmembrane voltage and controlling gating. To fill this void, we have used a strongly cationic, mutated mu-conotoxin peptide, which only partially blocks current through voltage-dependent sodium channels, to study voltage-dependent activation gating in both bound and unbound channels. When the peptide binds to the ion-conducting pore, it inhibit channel opening, necessitating stronger depolarization for channel activation. We show that this activation shift could result entirely from electrostatic inhibition of the movement of the voltage-sensing S4 charges and estimate the approximate physical distance through which the S4 charges move.

Structural model of the outer vestibule and selectivity filter of the Shaker voltage-gated K+ channel

A new generation of structural models were developed of the outer vestibule and ion-selective portion of the voltage-gated Shaker K+ channel. Some features of these models are similar to those that we have developed previously [Durrel S. R. and Guy H. R. (1992) Biophys. J. 62, 238-250; Guy H. R. (1990) In Monovalent Cations in Biological Systems (Pasternak C. A., Ed.), pp. 31-58, CRC Press, Boca Raton, FL; Guy H. R. and Durell S. R. (1994) In Molecular Evolution of Physiological processes (Fambrough D., Ed.), pp. 197-212, The Rockefeller University Press, NY; Guy H. R. and Durell S. R. (1995) In Ion Channels and Genetic Diseases (Dawson D., Ed.), pp. 1-16, The Rockefeller University Press, NY] and other features were modified to make the models more consistent with recent experimental findings. The first part of the P segment is postulated, as always, to form a short alpha helix that spans only the outer portion of the membrane. The helix is tilted so that its C-terminal is nearer the pore than its N-terminal. The latter part of the P segment, P2, is postulated to have a relatively elongated conformation that is positioned approximately parallel to the axis of the pore. Four of the P2 segments assemble to form an ion-selective region that has two narrow regions; one formed by the Y445 side-chains at the outer entrance of the pore and one formed by the backbone of the T442 residues near the innermost part of the P segments. The S6 segment is postulated to form two alpha helices. The first S6 helix packs next to the P segments in our models. The NMR structures of two scorpion toxins, charybdotoxin and agitoxin 2, have been docked into the models of the outer vestibules. The shape of the outer vestibule has been modeled so that specific toxin-channel residue-residue interactions correspond to those that have been identified experimentally.

Eight potassium channel families revealed by the C. elegans genome project

The wealth of accumulating data from the Caenorhabditis elegans genome sequencing project has rapidly accelerated the discovery of novel potassium channel genes and now places within reach the possibility of describing the total complement of potassium channels used by an individual species. Using annotated GenBank sequences, BLAST searches of unfinished sequences and degenerate oligonucleotide polymerase chain reaction (PCR) screens, we have identified and compiled genes for 38 C. elegans potassium channel and two cyclic nucleotide-gated cation channel subunits, representing eight conserved multigene families. Novel families of potassium channel genes were revealed, as well as conserved homologues of all known vertebrate families. Two separate families represent C. elegans homologues for human potassium channels recently implicated in hereditary long QT arrhythmias. Of particular note is an exceptionally large class of at least 23 genes with a novel subunit structure having two tandem 'P' domains; these channels may form as dimers in contrast to all other potassium channel types which form as tetramers. The 40 potassium channel genes are evenly distributed on all six C. elegans chromosomes, with the exception of the instances of gene clustering on the fifth and X chromosomes.