Mapping the membrane topography of the TH6–TH7 segment of the diphtheria toxin T-domain channel

Low pH triggers the translocation domain of diphtheria toxin (T-domain), which contains 10 α helices, to insert into a planar lipid bilayer membrane, form a transmembrane channel, and translocate the attached catalytic domain across the membrane. Three T-domain helices, corresponding to TH5, TH8, and TH9 in the aqueous crystal structure, form transmembrane segments in the open-channel state; the amino-terminal region, TH1–TH4, translocates across the membrane to the trans side. Residues near either end of the TH6–TH7 segment are not translocated, remaining on the cis side of the membrane; because the intervening 25-residue sequence is too short to form a transmembrane α-helical hairpin, it was concluded that the TH6–TH7 segment resides at the cis interface. Now we have examined this segment further, using the substituted-cysteine accessibility method. We constructed a series of 18 mutant T-domains with single cysteine residues at positions in TH6–TH7, monitored their channel formation in planar lipid bilayers, and probed for an effect of thiol-specific reagents on the channel conductance. For 10 of the mutants, the reagent caused a change in the single-channel conductance, indicating that the introduced cysteine residue was exposed within the channel lumen. For several of these mutants, we verified that the reactions occurred primarily in the open state, rather than in the flicker-closed state. We also established that blocking of the channel by an amino-terminal hexahistidine tag could protect mutants from reaction. Finally, we compared the reaction rates of reagent added to the cis and trans sides to quantify the residue’s accessibility from either side. This analysis revealed abrupt changes in cis- versus trans-side accessibility, suggesting that the TH6–TH7 segment forms a constriction that occupies a small portion of the total channel length. We also determined that this constriction is located near the middle of the TH8 helix.     

Analyzing topography of membrane-inserted diphtheria toxin T domain using BODIPY-streptavidin: at low pH, helices 8 and 9 form a transmembrane hairpin but helices 5-7 form stable nonclassical inserted segments on the cis side of the bilayer

Low pH-induced membrane insertion by diphtheria toxin T domain is crucial for A chain translocation into the cytoplasm. To define the membrane topography of the T domain, the exposure of biotinylated Cys residues to the cis and trans bilayer surfaces was examined using model membrane vesicles containing a deeply inserted T domain. To do this, the reactivity of biotin with external and vesicle-entrapped BODIPY-labeled streptavidin was measured. The T domain was found to insert with roughly 70-80% of the molecules in the physiologically relevant orientation. In this orientation, residue 349, located in the loop between hydrophobic helices 8 and 9, was exposed to the trans side of the bilayer, while other solution-exposed residues along the hydrophobic helices 5-9 region of the T domain located near the cis surface. A protocol developed to detect the movement of residues back and forth across the membranes demonstrated that T domain sequences did not rapidly equilibrate between the cis and the trans sides of the bilayer. Binding streptavidin to biotinylated residues prior to membrane insertion only inhibited T domain pore formation for residues in the loop between helices 8 and 9. Pore formation experiments used an approach avoiding interference from transient membrane defects/leakage that may occur upon the initial insertion of protein. Combined, these results indicate that at low pH hydrophobic helices 8 and 9 form a transmembrane hairpin, while hydrophobic helices 5-7 form a nonclassical deeply inserted nontransmembraneous state. We propose that this represents a novel pre-translocation state that is distinct from a previously defined post-translocation state.     

Conformation of the closed channel state of colicin A in proteoliposomes: an umbrella model

Colicin A (ColA) is a water-soluble toxin that forms a voltage-gated channel in the cytoplasmic membrane of Escherichia coli. Until now, two models were proposed for the closed channel state: the umbrella model and the penknife model. Mutants of ColA, each containing a single cysteine, were labeled with a nitroxide spin label, reconstituted into liposomes, and studied by electron paramagnetic resonance (EPR) spectroscopy to study the membrane-bound closed channel state. The spin-labeled ColA variants in solution and in liposomes of native E. coli lipid composition were analyzed in terms of the mobility of the nitroxide, its accessibility to paramagnetic reagents, and the polarity of its microenvironment. The EPR data determined for the soluble ColA pore-forming domain are in agreement with its crystal structure. Moreover, the EPR results show that ColA has a conformation in liposomes different from its water-soluble conformation. Residues that belong to helices H8 and H9 are significantly accessible for O₂ but not for nickel-ethylene diamine diacetic acid, indicating their location inside the membrane. In addition, the polarity values determined from the hyperfine tensor component A_zz of residues 176, 181, and 183 (H9) indicate the location of these residues close to the center of the lipid bilayer, supporting a transmembrane orientation of the hydrophobic hairpin. Furthermore, the accessibility and polarity data suggest that the spin-labeled side chains of the amphipathic helices (H1-H7 and H10) are located at the membrane-water interface. Evidence that the conformation of the closed channel state in artificial liposomes depends on lipid composition is given. The EPR results for ColA reconstituted into liposomes of E. coli lipids support the umbrella model for the closed channel state.     

Solid-state NMR studies of the membrane-bound closed state of the colicin E1 channel domain in lipid bilayers.

The colicin E1 channel polypeptide was shown to be organized anisotropically in membranes by solid-state NMR analysis of samples of uniformly 15N-labeled protein in oriented planar phospholipid bilayers. The 190 residue C-terminal colicin E1 channel domain is the largest polypeptide to have been characterized by 15N solid-state NMR spectroscopy in oriented membrane bilayers. The 15N-NMR spectra of the colicin E1 show that: (1) the structure and dynamics are independent of anionic lipid content in both oriented and unoriented samples; (2) assuming the secondary structure of the polypeptide is helical, there are both trans-membrane and in-plane helical segments; (3) trans-membrane helices account for approximately 20-25% of the channel polypeptide, which is equivalent to 38-48 residues of the 190-residue polypeptide. The results of the two-dimensional PISEMA spectrum are interpreted in terms of a single trans-membrane helical hairpin inserted into the bilayer from each channel molecule. These data are also consistent with this helical hairpin being derived from the 38-residue hydrophobic segment near the C-terminus of the colicin E1 channel polypeptide.     

Lipid-destabilizing properties of the hydrophobic helices H8 and H9 from colicin E1

Colicins are toxic proteins produced by Escherichia coli that must cross the membrane to exert their activity. The lipid insertion of their pf domain is linked to a conformational change which enables the penetration of a hydrophobic hairpin. They provide useful models to more generally study insertion of proteins, channel formation and protein translocation in and across membranes. In this paper, we study the lipid-destabilizing properties of helices H8 and H9 forming the hydrophobic hairpin of colicin E1. Modelling analysis suggests that those fragments behave like tilted peptides. The latter are characterized by an asymmetric distribution of their hydrophobic residues when helical. They are able to interact with a hydrophobic/hydrophilic interface (such as a lipid membrane) and to destabilize the organized system into which they insert. Fluorescence techniques using labelled liposomes clearly show that H9, and H8 to a lesser extent, destabilize lipid particles, by inducing fusion and leakage. AFM assays clearly indicate that H8 and especially H9 induce membrane fragilization. Holes in the membrane are even observed in the presence of H9. This behaviour is close to what is seen with viral fusion peptides. Those results suggest that the peptides could be involved in the toroidal pore formation of colicin E1, notably by disturbing the lipids and facilitating the insertion of the other, more hydrophilic, helices that will form the pore. Since tilted, lipid-destabilizing fragments are also common to membrane proteins and to signal sequences, we suggest that tilted peptides should have an ubiquitous role in the mechanism of insertion of proteins into membranes.     

Probing the Structure of the Diphtheria Toxin Channel : Reactivity in Planar Lipid Bilayer Membranes of Cysteine-substituted Mutant Channels with Methanethiosulfonate Derivatives

Previous work has established that the 61 amino acid stretch from residue 322 to 382 in the T-domain of diphtheria toxin forms channels indistinguishable in ion-conducting properties from those formed by the entire T-domain. In the crystal structure of the toxin''s water-soluble form, the bulk of this stretch is an α-helical hairpin, designated TH8-9. The present study was directed at determining which residues in TH8-9 line the ion-conducting pathway of the channel; i.e., its lumen or entrances. To this end, we singly mutated 49 of TH8-9''s 51 residues (328–376) to cysteines, formed channels with the mutant T-domain proteins in planar lipid bilayers, and then determined whether they reacted with small, charged, lipid-insoluble, sulfhydryl-specific methanethiosulfonate (MTS) derivatives added to the bathing solutions. The indication of a reaction, and that the residue lined the ion-conducting pathway, was a sudden change in single-channel conductance and/or flickering behavior. The results of this study were surprising in two respects. First, of the 49 cysteine-substituted residues in TH8-9 tested, 23 reacted with MTS derivatives in a most unusual pattern consisting of two segments: one extending from 329 to 341 (11 of 13 reacted), and the other from 347 to 359 (12 of 13 reacted); none of the residues outside of these two segments appeared to react. Second, in every cysteine mutant channel manifesting an MTS effect, only one transition in single-channel conductance (or flickering behavior) occurred, not the several expected for a multimeric channel. Our results are not consistent with an α-helical or β-strand model for the channel, but instead suggest an open, flexible structure. Moreover, contrary to common sense, they indicate that the channel is not multimeric but is formed from only one TH8-9 unit of the T-domain.     

Membrane Partitioning of the Pore-Forming Domain of Colicin A. Role of the Hydrophobic Helical Hairpin

The colicins are bacteriocins that target Escherichia coli and kill bacterial cells through different mechanisms. Colicin A forms ion channels in the inner membranes of nonimmune bacteria. This activity resides exclusively in its C-terminal fragment (residues 387–592). The soluble free form of this domain is a 10 α-helix bundle. The hydrophobic helical hairpin, H8–H9, is buried inside the structure and shielded by eight amphipathic surface helices. The interaction of the C-terminal colicin A domain and several chimeric variants with lipidic vesicles was examined here by isothermal titration calorimetry. In the mutant constructions, natural sequences of the hydrophobic helices H8 and H9 were either removed or substituted by polyalanine or polyleucine. All the constructions fully associated with DOPG liposomes including the mutant that lacked helices H8 and H9, indicating that amphipathic rather than hydrophobic helices were the major determinants of the exothermic binding reactions. Alanine is not specially favored in the lipid-bound form; the chimeric construct with polyalanine produced lower enthalpy gain. On the other hand, the large negative heat capacities associated with partitioning, a characteristic feature of the hydrophobic effect, were found to be dependent on the sequence hydrophobicity of helices H8 and H9.     

Lipid-destabilizing properties of the hydrophobic helices H8 and H9 from colicin E1

Colicins are toxic proteins produced by Escherichia coli that must cross the membrane to exert their activity. The lipid insertion of their pf domain is linked to a conformational change which enables the penetration of a hydrophobic hairpin. They provide useful models to more generally study insertion of proteins, channel formation and protein translocation in and across membranes. In this paper, we study the lipid-destabilizing properties of helices H8 and H9 forming the hydrophobic hairpin of colicin E1. Modelling analysis suggests that those fragments behave like tilted peptides. The latter are characterized by an asymmetric distribution of their hydrophobic residues when helical. They are able to interact with a hydrophobic/hydrophilic interface (such as a lipid membrane) and to destabilize the organized system into which they insert. Fluorescence techniques using labelled liposomes clearly show that H9, and H8 to a lesser extent, destabilize lipid particles, by inducing fusion and leakage. AFM assays clearly indicate that H8 and especially H9 induce membrane fragilization. Holes in the membrane are even observed in the presence of H9. This behaviour is close to what is seen with viral fusion peptides. Those results suggest that the peptides could be involved in the toroidal pore formation of colicin E1, notably by disturbing the lipids and facilitating the insertion of the other, more hydrophilic, helices that will form the pore. Since tilted, lipid-destabilizing fragments are also common to membrane proteins and to signal sequences, we suggest that tilted peptides should have an ubiquitous role in the mechanism of insertion of proteins into membranes.     

The C-terminal half of the colicin A pore-forming domain is active in vivo and in vitro

The pore-forming domain of colicin A (pfColA) fused to a prokaryotic signal peptide (sp-pfColA) is transported across and inserts into the inner membrane of Escherichia coli from the periplasmic side and forms a functional channel. The soluble structure of pfColA consists of a ten-helix bundle containing a hydrophobic helical hairpin. Here, we generated a series of mutants in which an increasing number of sp-pfColA alpha-helices was deleted. These peptides were tested for their ability to form ion channels in vivo and in vitro. We found that the shortest sp-pfColA mutant protein that killed Escherichia coli was composed of the five last alpha-helices of sp-pfColA, whereas the shortest peptide that formed a channel in planar lipid bilayer membranes similar to that of intact pfColA was the protein composed of the last six alpha-helices. The peptide composed of the last five alpha-helices of pfColA generated a voltage-independent conductance in planar lipid bilayer with properties very different from that of intact pfColA. Thus, helices 1 to 4 are unnecessary for channel formation, while helix 5, or some part of it, is important but not absolutely necessary. Voltage-dependence of colicin is evidently controlled by the first four alpha-helices of pfColA.     

Transmembrane insertion of the Colicin Ia hydrophobic hairpin

Colicin Ia is a bactericidal protein that forms voltage-dependent, ion-conducting channels, both in the inner membrane of target bacteria and in planar bilayer membranes. Its amino acid sequence is rich in charged residues, except for a hydrophobic segment of 40 residues near the carboxyl terminus. In the crystal structure of colicin Ia and related colicins, this segment forms an α-helical hairpin. The hydrophobic segment is thought to be involved in the initial association of the colicin with the membrane and in the formation of the channel, but various orientations of the hairpin with respect to the membrane have been proposed. To address this issue, we attached biotin to a residue at the tip of the hydrophobic hairpin, and then probed its location with the biotin-binding protein streptavidin, added to one side or the other of a planar bilayer. Streptavidin added to the same side as the colicin prevented channel opening. Prior addition of streptavidin to the opposite side protected channels from this effect, and also increased the rate of channel opening; it produced these effects even before the first opening of the channels. These results suggest a model of membrane association in which the colicin first binds with the hydrophobic hairpin parallel to the membrane; next the hairpin inserts in a transmembrane orientation; and finally the channel opens. We also used streptavidin binding to obtain a stable population of colicin molecules in the membrane, suitable for the quantitative study of voltage-dependent gating. The effective gating charge thus determined is pH-independent and relatively small, compared with previous results for wild-type colicin Ia. Received: 12 November 1996/Revised: 23 January 1997     

Oligomeric Structure of Colicin Ia Channel in Lipid Bilayer Membranes

Colicin Ia is a soluble, harpoon-shaped bacteriocin which translocates across the periplasmic space of sensitive Escherichia coli cell by parasitizing an outer membrane receptor and forms voltage-gated ion channels in the inner membrane. This process leads to cell death, which has been thought to be caused by a single colicin Ia molecule. To directly visualize the three-dimensional structure of the channel, we generated two-dimensional crystals of colicin Ia inserted in lipid-bilayer membranes and determined a ∼17 three-dimensional model by electron crystallography. Supported by velocity sedimentation, chemical cross-linking and single-particle image analysis, the three-dimensional structure is a crown-shaped oligomer enclosing a ∼35 Å-wide extrabilayer vestibule. Our study suggests that lipid insertion instigates a global conformational change in colicin Ia and that more than one molecule participates in the channel architecture with the vestibule, possibly facilitating the known large scale peptide translocation upon channel opening.Colicin Ia is a pore-forming water-soluble bacterial toxin produced by some strains of Escherichia coli to kill other competing bacteria (1, 2). It belongs to a functionally and structurally similar group of proteins that also includes colicins A (3), E1 (4), and N (5). Each of these proteins consist of three domains with distinct properties; the receptor domain (R), which binds a specific outer membrane receptor on the target cell, and the translocation domain (T) at the N terminus, responsible for traversing the outer membrane and the periplasmic space to deliver the channel-forming domain (C) at the C terminus to the bacterial inner membrane. The bundle of 10 α-helices that compose the C domain changes its conformation to form a voltage-gated ion channel in the plasma membrane. Opening of the channel produces an efflux of ions that depletes the cellular energy resources and ultimately leads to cell death.The x-ray structure of full-length, soluble colicin Ia (69 kDa) has been determined (6). The monomeric molecule is mostly α-helical, with the R domain separated from the T and C domains by a pair of unusually long (∼160 Å) α-helices thought possibly to span the periplasmic space during channel formation (6). The C domain is characterized by two hydrophobic helices (VIII and IX; residues Ala-580—Ile-612) that is surrounded by the remaining eight largely amphipathic α-helices. The same structural motif for the C domain is conserved in other members of the colicin family and is also present in the channel-forming domains of diphtheria toxin, exotoxin A, and the Bcl family of pro- and anti-apoptotic proteins (7). This pair of helices, termed the hydrophobic hairpin, is instrumental in driving the initial membrane insertion event (8) that is followed by a series of large scale pH and voltage-dependent conformational changes in the C domain, resulting in the opening of the ion channel in the plasma membrane (9, 10). In the absence of a high resolution membrane-inserted structure of a channel-forming colicin, solid-state NMR (11, 12), streptavidin binding (8) and cross-linking of site-directed cysteine mutants (9) have suggested that the initial membrane-bound intermediate exists as a two-dimensional helical array of the eight amphipathic helices (I-VII and X) spread across the membrane surface, with the hydrophobic helices (VIII and IX) embedded in the bilayer. A recent electron paramagnetic resonance study using preparations of spin-labeled ColA proteoliposomes has supported a similar umbrella model where the eight amphipathic helices reside at the air-water interface for the closed-channel state (13). Biotin-labeled cysteine mutants have also been used to determine how much of the C domain (aside from the hydrophobic hairpin) crosses the plasma membrane (14, 15) for colicin Ia. A large region of the amphipathic sequence (helices II-V; residues Leu-474—Tyr-541) has been found to cross from the cis to the trans side of the membrane in planar lipid bilayer experiments, resulting in a four-transmembrane segment molecule that is thought to form the ion channel.Because the 12–13 residue α-helices of the C domain are well short of the ∼20 residues required to span the plasma membrane, it has been proposed that conformational changes causing helix extension take place during the channel formation process. ¹³C spin diffusion NMR has indicated that whereas the overall secondary structure of the C domain is preserved, most of the helices undergo “opening,” and modulation of the tertiary structure allows for the required extension of the helices to cross the plasma membrane and form the channel (16). The internal structure of the colicin Ia channel has been investigated by examining the effect of different nonelectrolyte molecules on the single-channel conductance in planar lipid bilayer membranes (17). It was determined that the diameter at the cis entrance (equivalent to the outside of the cell) is 18 Å, and the diameter at the trans entrance (inside the membrane) is 10 Å, with a 7 Å diameter constriction located in close proximity to the trans entrance of the channel. More recent studies (18) employing the substituted cysteine accessibility method to determine what residues line the open colicin Ia channel suggest an hourglass-shaped pore with the most constricted part near the cis rather than the trans side, as opposed to the conclusion of Krasilnikov et al. (17). Both studies point to a pore constriction inside the membrane, and as pointed out by Kienker et al. 18), there exist plausible explanations to reconcile some of the differing results. The large diameter of the colicin Ia channel coupled with the studies which indicate that each colicin Ia molecule contributes four transmembrane segments in the membrane integrated state (14) suggests that the ion channel is formed by a multimer of colicin Ia molecules. However, all of the past studies directed at determining the oligomeric state of any of the colicin channels indicate a monomeric structure. The question as to how a four-transmembrane monomeric protein can form an ion channel of sufficient diameter to allow the passage of ions as large as tetraethyl ammonium (19) has remained unanswered.In this work we have subjected colicin Ia incorporated into lipid bilayer membranes to structural and biochemical investigations. We show, based on cross-linking and velocity sedimentation experiments, single-particle analysis of electron micrographs and results from electron crystallographic analysis of two-dimensional crystals of colicin Ia that the protein forms oligomers upon insertion into the bilayer. The suggested architecture of this oligomer based on the ∼17 Å resolution three-dimensional model and the biological implications, are discussed.     

Topography of helices 5-7 in membrane-inserted diphtheria toxin T domain: identification and insertion boundaries of two hydrophobic sequences that do not form a stable transmembrane hairpin

The T domain of diphtheria toxin undergoes a low pH-induced conformational change that allows it to penetrate cell membranes. T domain hydrophobic helices 8 and 9 can adopt two conformations, one close to the membrane surface (P state) and a second in which they apparently form a transmembrane hairpin (TM state). We have now studied T domain helices 5-7, a second cluster of hydrophobic helices, using Cys-scanning mutagenesis. After fluorescently labeling a series of Cys residues, penetration into a non-polar environment, accessibility to externally added antibodies, and relative depth in the bilayer were monitored. It was found that helices 5-7 insert shallowly in the P state and deeply in the TM state. Thus, the conformational changes in helices 5-7 are both similar and somehow linked to those in helices 8 and 9. The boundaries of deeply inserting sequences were also identified. One deeply inserted segment was found to span residues 270 to 290, which overlaps helix 5, and a second spanned residues 300 to 320, which includes most of helix 6 and all of helix 7. This indicates that helices 6 and 7 form a continuous hydrophobic segment despite their separation by a Pro-containing kink. Additionally, it is found that in the TM state some residues in the hydrophilic loop between helices 5 and 6 become more highly exposed than they are in the P state. Their exposure to external solution in the TM state indicates that helices 5-7 do not form a stable transmembrane hairpin. However, helix 5 and/or helices 6 plus 7 could form transmembrane structures that are in equilibrium with non-transmembrane states, or be kinetically prevented from forming a transmembrane structure. How helices 5-7 might influence the mechanism by which the T domain aids translocation of the diphtheria toxin A chain across membranes is discussed.     

Single streptomyces lividans K(+) channels: functional asymmetries and sidedness of proton activation.

Basic electrophysiological properties of the KcsA K(+) channel were examined in planar lipid bilayer membranes. The channel displays open-state rectification and weakly voltage-dependent gating. Tetraethylammonium blocking affinity depends on the side of the bilayer to which the blocker is added. Addition of Na(+) to the trans chamber causes block of open-channel current, while addition to the cis side has no effect. Most striking is the activation of KcsA by protons; channel activity is observed only when the trans bilayer chamber is at low pH. To ascertain which side of the channel faces which chamber, residues with structurally known locations were mapped to defined sides of the bilayer. Mutation of Y82, an external residue, results in changes in tetraethylammonium affinity exclusively from the cis side. Channels with cysteine residues substituted at externally exposed Y82 or internally exposed Q119 are functionally modified by methanethiosulfonate reagents from the cis or trans chambers, respectively. Block by charybdotoxin, known to bind to the channel's external mouth, is observed only when the toxin is added to the cis side of channels mutated to be toxin sensitive. These results demonstrate unambiguously that the protonation sites linked to gating are on the intracellular portion of the KcsA protein.     

Sizing the protein translocation pathway of colicin Ia channels

The bacterial toxin colicin Ia forms voltage-gated channels in planar lipid bilayers. The toxin consists of three domains, with the carboxy-terminal domain (C-domain) responsible for channel formation. The C-domain contributes four membrane-spanning segments and a 68-residue translocated segment to the open channel, whereas the upstream domains and the amino-terminal end of the C-domain stay on the cis side of the membrane. The isolated C-domain, lacking the two upstream domains, also forms channels; however, the amino terminus and one of the normally membrane-spanning segments can move across the membrane. (This can be observed as a drop in single-channel conductance.) In longer carboxy-terminal fragments of colicin Ia that include /=90 mV, even a 26-A stopper is translocated. Upon reduction of their disulfide bonds, all of the stoppers are easily translocated, indicating that it is the folded structure, rather than some aspect of the primary sequence, that slows translocation of the stoppers. Thus, the pathway for translocation is >/=26 A in diameter, or can stretch to this value. This is large enough for an alpha-helical hairpin to fit through.     

Protein Translocation across Planar Bilayers by the Colicin Ia Channel-Forming Domain: Where Will It End?

Colicin Ia, a 626-residue bactericidal protein, consists of three domains, with the carboxy-terminal domain (C domain) responsible for channel formation. Whole colicin Ia or C domain added to a planar lipid bilayer membrane forms voltage-gated channels. We have shown previously that the channel formed by whole colicin Ia has four membrane-spanning segments and an approximately 68-residue segment translocated across the membrane. Various experimental interventions could cause a longer or shorter segment within the C domain to be translocated, making us wonder why translocation normally stops where it does, near the amino-terminal end of the C domain (approximately residue 450). We hypothesized that regions upstream from the C domain prevent its amino-terminal end from moving into and across the membrane. To test this idea, we prepared C domain with a ligand attached near its amino terminus, added it to one side of a planar bilayer to form channels, and then probed from the opposite side with a water-soluble protein that can specifically bind the ligand. The binding of the probe had a dramatic effect on channel gating, demonstrating that the ligand (and hence the amino-terminal end of the C domain) had moved across the membrane. Experiments with larger colicin Ia fragments showed that a region of more than 165 residues, upstream from the C domain, can also move across the membrane. All of the colicin Ia carboxy-terminal fragments that we examined form channels that pass from a state of relatively normal conductance to a low-conductance state; we interpret this passage as a transition from a channel with four membrane-spanning segments to one with only three.     

Behavior of diphtheria toxin T domain containing substitutions that block normal membrane insertion at Pro345 and Leu307: control of deep membrane insertion and coupling between deep insertion of hydrophobic subdomains

Diphtheria toxin T domain aids the translocation of toxin A chain across membranes. T domain has two hydrophobic layers/subdomains that can insert deeply into membranes: helices TH8 and 9, which form a transmembrane hairpin, and helices TH5-7, which form a nonclassical, nontransmembrane structure. Substitutions were made at Pro345, a residue located near the turn between TH8 and 9. P345 is critical for toxicity and pore formation by the T domain. Fluorescence methods showed that hairpin-disrupting Gly or Glu substitutions at 345 did not insert into lipid bilayers as deeply as the wild-type protein, and consistent with previous studies, these mutations reduced pore formation activity as assayed by a novel biotin-streptavidin-based influx assay. Introducing Pro at positions 347 or 353 not only failed to compensate for substitutions at P345, but also they further disrupted deep insertion and/or pore formation. Substitution of P345 with Asn, a residue that promotes helical hairpin formation almost as well as Pro, resulted in somewhat more normal insertion and pore formation than other substitutions. Importantly, a P345E substitution disrupted deep insertion of TH5-7. This suggests that TH8 and 9 and TH5-7 undergo some sort of coordinated insertion into the lipid bilayer and/or that the membrane-inserted T domain has a distinct tertiary structure in which TH5-7 interact with TH8 and 9 instead of consisting of noninteracting hydrophobic segments. Intriguingly, a L307R substitution in TH6, which disrupted deep insertion of TH7, had only a weak effect on pore formation and deep insertion of TH8 and 9. This suggests that the TH8 and 9 region can insert independently of TH5-7 to some degree and that TH8 and 9 insertion may occur early in T-domain insertion.     

Identification of a translocated gating charge in a voltage-dependent channel. Colicin E1 channels in planar phospholipid bilayer membranes.

The availability of primary sequences for ion-conducting channels permits the development of testable models for mechanisms of voltage gating. Previous work on planar phospholipid bilayers and lipid vesicles indicates that voltage gating of colicin E1 channels involves translocation of peptide segments of the molecule into and across the membrane. Here we identify histidine residue 440 as a gating charge associated with this translocation. Using site-directed mutagenesis to convert the positively charged His440 to a neutral cysteine, we find that the voltage dependence for turn-off of channels formed by this mutant at position 440 is less steep than that for wild-type channels; the magnitude of the change in voltage dependence is consistent with residue 440 moving from the trans to the cis side of the membrane in association with channel closure. The effect of trans pH changes on the ion selectivity of channels formed by the carboxymethylated derivative of the cysteine 440 mutant independently establishes that in the open channel state, residue 440 lies on the trans side of the membrane. On the basis of these results, we propose that the voltage-gated opening of colicin E1 channels is accompanied by the insertion into the bilayer of a helical hairpin loop extending from residue 420 to residue 459, and that voltage-gated closing is associated with the extrusion of this loop from the interior of the bilayer back to the cis side.     

Major transmembrane movement associated with colicin Ia channel gating

Colicin Ia, a bacterial protein toxin of 626 amino acid residues, forms voltage-dependent channels in planar lipid bilayer membranes. We have exploited the high affinity binding of streptavidin to biotin to map the topology of the channel-forming domain (roughly 175 residues of the COOH-terminal end) with respect to the membrane. That is, we have determined, for the channel's open and closed states, which parts of this domain are exposed to the aqueous solutions on either side of the membrane and which are inserted into the bilayer. This was done by biotinylating cysteine residues introduced by site-directed mutagenesis, and monitoring by electrophysiological methods the effect of streptavidin addition on channel behavior. We have identified a region of at least 68 residues that flips back and forth across the membrane in association with channel opening and closing. This identification was based on our observations that for mutants biotinylated in this region, streptavidin added to the cis (colicin- containing) compartment interfered with channel opening, and trans streptavidin interfered with channel closing. (If biotin was linked to the colicin by a disulfide bond, the effects of streptavidin on channel closing could be reversed by detaching the streptavidin-biotin complex from the colicin, using a water-soluble reducing agent. This showed that the cysteine sulfur, not just the biotin, is exposed to the trans solution). The upstream and downstream segments flanking the translocated region move into and out of the bilayer during channel opening and closing, forming two transmembrane segments. Surprisingly, if any of several residues near the upstream end of the translocated region is held on the cis side by streptavidin, the colicin still forms voltage-dependent channels, indicating that a part of the protein that normally is fully translocated across the membrane can become the upstream transmembrane segment. Evidently, the identity of the upstream transmembrane segment is not crucial to channel formation, and several open channel structures can exist.     

Self-assembly of a simple membrane protein: coarse-grained molecular dynamics simulations of the influenza M2 channel

The transmembrane (TM) domain of the M2 channel protein from influenza A is a homotetrameric bundle of α-helices and provides a model system for computational approaches to self-assembly of membrane proteins. Coarse-grained molecular dynamics (CG-MD) simulations have been used to explore partitioning into a membrane of M2 TM helices during bilayer self-assembly from lipids. CG-MD is also used to explore tetramerization of preinserted M2 TM helices. The M2 helix monomer adopts a membrane spanning orientation in a lipid (DPPC) bilayer. Multiple extended CG-MD simulations (5 × 5 μs) were used to study the tetramerization of inserted M2 helices. The resultant tetramers were evaluated in terms of the most populated conformations and the dynamics of their interconversion. This analysis reveals that the M2 tetramer has 2× rotationally symmetrical packing of the helices. The helices form a left-handed bundle, with a helix tilt angle of ∼16°. The M2 helix bundle generated by CG-MD was converted to an atomistic model. Simulations of this model reveal that the bundle's stability depends on the assumed protonation state of the H37 side chains. These simulations alongside comparison with recent x-ray (3BKD) and NMR (2RLF) structures of the M2 bundle suggest that the model yielded by CG-MD may correspond to a closed state of the channel.     

Structures of the M2 channel-lining segments from nicotinic acetylcholine and NMDA receptors by NMR spectroscopy

The structures of functional peptides corresponding to the predicted channel-lining M2 segments of the nicotinic acetylcholine receptor (AChR) and of a glutamate receptor of the NMDA subtype (NMDAR) were determined using solution NMR experiments on micelle samples, and solid-state NMR experiments on bilayer samples. Both M2 segments form straight transmembrane alpha-helices with no kinks. The AChR M2 peptide inserts in the lipid bilayer at an angle of 12 degrees relative to the bilayer normal, with a rotation about the helix long axis such that the polar residues face the N-terminal side of the membrane, which is assigned to be intracellular. A model built from these solid-state NMR data, and assuming a symmetric pentameric arrangement of M2 helices, results in a funnel-like architecture for the channel, with the wide opening on the N-terminal intracellular side.