On the role of lipid in colicin pore formation

Insights into the protein-membrane interactions by which the C-terminal pore-forming domain of colicins inserts into membranes and forms voltage-gated channels, and the nature of the colicin channel, are provided by data on: (i) the flexible helix-elongated state of the colicin pore-forming domain in the fluid anionic membrane interfacial layer, the optimum anionic surface charge for channel formation, and voltage-gated translocation of charged regions of the colicin domain across the membrane; (ii) structure-function data on the voltage-gated K(+) channel showing translocation of an arginine-rich helical segment through the membrane; (iii) toroidal channels formed by small peptides that involve local participation of anionic lipids in an inverted phase. It is proposed that translocation of the colicin across the membrane occurs through minimization of the Born charging energy for translocation of positively charged basic residues across the lipid bilayer by neutralization with anionic lipid head groups. The resulting pore structure may consist of somewhat short, ca. 16 residues, trans-membrane helices, in a locally thinned membrane, together with surface elements of inverted phase lipid micelles.     

Solid-state NMR investigation of the dynamics of the soluble and membrane-bound colicin Ia channel-forming domain.

Solid-state NMR spectroscopy was employed to study the molecular dynamics of the colicin Ia channel domain in the soluble and membrane-bound states. In the soluble state, the protein executes small-amplitude librations (with root-mean-square angular fluctuations of 0-10 degrees ) in the backbone and larger-amplitude motions (16-17 degrees ) in the side chains. Upon membrane binding, the motional amplitudes increase significantly for both the backbone (12-16 degrees ) and side chains (23-29 degrees ), as manifested by the reduction in the C-H and H-H dipolar couplings and (15)N chemical shift anisotropy. These motions occur not only on the pico- to nanosecond time scales, but also on the microsecond time scale, as revealed by the (1)H rotating-frame spin-lattice relaxation times. Average motional correlation times of 0.8 and 1.2 micros were extracted for the soluble and membrane-bound states, respectively. In comparison, both forms of the colicin Ia channel domain are completely immobile on the millisecond scale. These results indicate that the colicin Ia channel domain has enhanced conformational mobility in the lipid bilayer compared to the soluble state. This membrane-induced mobility increase is consistent with the loss of tertiary structure of the protein in the membrane, which was previously suggested by the extended helical array model [Zakharov et al. (1998) Proc. Natl. Acad. Sci. U.S.A. 95, 4282-4287]. An extended structure would also facilitate protein interactions with the mobile lipids and thus increase the protein internal motions. We speculate that the large mobility of the membrane-bound colicin Ia channel domain is a prerequisite for channel opening in the presence of a voltage gradient.     

Colicin crystal structures: pathways and mechanisms for colicin insertion into membranes

The X-ray structures of the channel-forming colicins Ia and N, and endoribonucleolytic colicin E3, as well as of the channel domains of colicins A and E1, and spectroscopic and calorimetric data for intact colicin E1, are discussed in the context of the mechanisms and pathways by which colicins are imported into cells. The extensive helical coiled-coil in the R domain and internal hydrophobic hairpin in the C domain are important features relevant to colicin import and channel formation. The concept of outer membrane translocation mediated by two receptors, one mainly used for initial binding and second for translocation, such as BtuB and TolC, respectively, is discussed. Helix elongation and conformational flexibility are prerequisites for import of soluble toxin-like proteins into membranes. Helix elongation contradicts suggestions that the colicin import involves a molten globule intermediate. The nature of the open-channel structure is discussed.     

Colicin crystal structures: pathways and mechanisms for colicin insertion into membranes

The X-ray structures of the channel-forming colicins Ia and N, and endoribonucleolytic colicin E3, as well as of the channel domains of colicins A and E1, and spectroscopic and calorimetric data for intact colicin E1, are discussed in the context of the mechanisms and pathways by which colicins are imported into cells. The extensive helical coiled-coil in the R domain and internal hydrophobic hairpin in the C domain are important features relevant to colicin import and channel formation. The concept of outer membrane translocation mediated by two receptors, one mainly used for initial binding and second for translocation, such as BtuB and TolC, respectively, is discussed. Helix elongation and conformational flexibility are prerequisites for import of soluble toxin-like proteins into membranes. Helix elongation contradicts suggestions that the colicin import involves a molten globule intermediate. The nature of the open-channel structure is discussed.     

The cytotoxic domain of colicin E9 is a channel-forming endonuclease

Bacterial toxins commonly translocate cytotoxic enzymes into cells using channel-forming subunits or domains as conduits. Here we demonstrate that the small cytotoxic endonuclease domain from the bacterial toxin colicin E9 (E9 DNase) shows nonvoltage-gated, channel-forming activity in planar lipid bilayers that is linked to toxin translocation into cells. A disulfide bond engineered into the DNase abolished channel activity and colicin toxicity but left endonuclease activity unaffected; NMR experiments suggest decreased conformational flexibility as the likely reason for these alterations. Concomitant with the reduction of the disulfide bond is the restoration of conformational flexibility, DNase channel activity and colicin toxicity. Our data suggest that endonuclease domains of colicins may mediate their own translocation across the bacterial inner membrane through an intrinsic channel activity that is dependent on structural plasticity in the protein.     

Structure of colicin I receptor bound to the R-domain of colicin Ia: implications for protein import

Colicin Ia is a 69 kDa protein that kills susceptible Escherichia coli cells by binding to a specific receptor in the outer membrane, colicin I receptor (70 kDa), and subsequently translocating its channel forming domain across the periplasmic space, where it inserts into the inner membrane and forms a voltage-dependent ion channel. We determined crystal structures of colicin I receptor alone and in complex with the receptor binding domain of colicin Ia. The receptor undergoes large and unusual conformational changes upon colicin binding, opening at the cell surface and positioning the receptor binding domain of colicin Ia directly above it. We modelled the interaction with full-length colicin Ia to show that the channel forming domain is initially positioned 150 A above the cell surface. Functional data using full-length colicin Ia show that colicin I receptor is necessary for cell surface binding, and suggest that the receptor participates in translocation of colicin Ia across the outer membrane.     

Structure and dynamics of the colicin E1 channel

The toxin-like and bactericidal colicin E1 molecule is of interest for problems of toxin action, polypeptide translocation across membranes, voltage-gated channels, and receptor function. Colicin E1 binds to a receptor in the outer membrane and is translocated across the cell envelope to the inner membrane. Import of the colicin channel-forming domain into the inner membrane involves a translocation-competent intermediate state and a membrane potential-dependent movement of one third to one half of the channel peptide into the membrane bilayer. The voltage-gated channel has a conductance sufficiently large to depolarize the Escherichia coli cytoplasmic membrane. Amino acid residues that affect the channel ion selectivity have been identified by site-directed mutagenesis. The colicin E1 channel is one of a few membrane proteins whose secondary structures in the membrane, predominantly alpha-helix, have been determined by physico-chemical techniques. Hypothesis for the identity of the trans-membrane helices, and the mechanism of binding to the membrane, are influenced by the solved crystal structure of the soluble colicin A channel peptide. The protective action of immunity protein is a unique aspect of the colicin problem, and information has been obtained, by genetic techniques, about the probable membrane topography of the imm gene product.     

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.     

Unfolding pathway of the colicin E1 channel protein on a membrane surface

The channel-forming domain of colicin E1 is composed of a soluble helical bundle which, upon membrane binding, unfolds to form an extended, two-dimensional helical net in the membrane interfacial layer. To characterize the pathway of unfolding of the protein and the structure of the surface-bound intermediate, the time-course of intra-protein distance changes and unfolding on a millisecond time-scale were determined from the kinetics of changes in the efficiency of fluorescence resonance energy transfer, and of the donor-acceptor overlap integral, between each of six individual tryptophan residues and a Cys-conjugated energy transfer acceptor (C509-AEDANS). Comparison of the rate constants revealed the following order of events associated with unfolding of the protein at the membrane surface: (A) movement of the hydrophobic core helices VIII-IX, coincident with a small change in Trp-Cys509 distances of the outer helices; (B) unfolding of surface helices in the helical bundle in the order: helix I, helices III, IV, VI, VII, and helix V; (C) a slow (time-scale, seconds) condensation of the surface-bound helices. The rate of protein unfolding events increased with increasing anionic lipid content. Unfolding did not occur below the lipid thermal phase transition, indicating that unfolding requires mobility in the interfacial layer. The structure of the two-dimensional membrane-bound intermediate in the steady-state was inferred to consist of a quasi-circular arrangement of eight helices embedded in the membrane interfacial layer and anchored by the hydrophobic helical hairpin. The pathway of unfolding of the colicin channel at the membrane surface, catalyzed by electrostatic and hydrophobic forces, is the first described for a membrane-active protein. It is proposed that the pathway and principles described for the colicin protein are relevant to membrane protein import.     

Histidine 440 controls the opening of colicin E1 channels in a lipid-dependent manner

The in vitro activity of many pore-forming toxins, in particular, the rate of increase in the membrane conductance induced by the channel-forming domain (P178) of colicin E1 is maximum at an acidic pH. However, after P178 binding at acidic conditions, a subsequent pH shift from 4 to 6 on both sides of the planar bilayer lipid membrane caused a large increase in the trans-membrane current which was solely due to an increase in the number of open channels. This effect required the presence of anionic lipid. Replacing the His440 residue of P178 by alanine eliminated the pH-shift effect thereby showing that it is associated with deprotonation of this histidine residue. It was concluded that alkalinization-induced weakening of the electrostatic interactions between colicin and the membrane surface facilitates conformational changes required for the transition of membrane-bound colicin molecules to an active channel state.     

Conformational changes of colicin Ia channel-forming domain upon membrane binding: a solid-state NMR study

Channel-forming colicins are bactericidal proteins that spontaneously insert into hydrophobic lipid bilayers. We have used magic-angle spinning solid-state nuclear magnetic resonance spectroscopy to examine the conformational differences between the water-soluble and the membrane-bound states of colicin Ia channel domain, and to study the effect of bound colicin on lipid bilayer structure and dynamics. We detected (13)C and (15)N isotropic chemical shift differences between the two forms of the protein, which indicate structural changes of the protein due to membrane binding. The Val C(alpha) signal, unambiguously assigned by double-quantum experiments, gave a 0.6 ppm downfield shift in the isotropic position and a 4 ppm reduction in the anisotropic chemical shift span after membrane binding. These suggest that the alpha-helices in the membrane-bound colicin adopt more ideal helical torsion angles as they spread onto the membrane. Colicin binding significantly reduced the lipid chain order, as manifested by (2)H quadrupolar couplings. These results are consistent with the model that colicin Ia channel domain forms an extended helical array at the membrane-water interface upon membrane binding.     

The molecular basis for the pH-activation mechanism in the channel-forming bacterial colicin E1

The in vitro activity of the channel-forming bacteriocins such as colicin E1 in model membranes requires the specific activation of the protein by an acidic environment in the presence of a membrane potential. Acid activation of the C-terminal domain results in the formation of an insertion-competent intermediate with an enhanced ability to penetrate and perforate cell membranes. We report novel findings of this activation process through the design and study of mutant proteins involving the replacement of conserved Asp residues Asp-408, Asp-410, and Asp-423 within helices 5a and 4 in the colicin E1 channel domain that resulted in enhanced membrane binding, bilayer insertion rates, and ion channel activities at near neutral pH values. This activation process involves the destabilization of a critical salt bridge (Asp-410 and Lys-406) and H-bonds (Asp-408 and Ser-405 main chain; Asp-423 and Lys-420 main chain). The helix-to-coil transition of this motif was identified previously by time-resolved Trp fluorescence measurements (Merrill, A. R., Steer, B. A., Prentice, G. A., Weller, M. J., and Szabo, A. G. (1997) Biochemistry 36, 6874-6884), and here we use this approach to demonstrate that disruption of the helical structure of helices 4 and 5a results in a shift in this equilibrium to favor the coil state. Finally, we show that the essential components of the pH trigger motif are conserved among the channel-forming colicins and that it likely exists within other bacterial proteins and may even have evolved into more sophisticated devices in a number of microbial species.     

Conformational changes of colicin Ia channel-forming domain upon membrane binding: a solid-state NMR study

Channel-forming colicins are bactericidal proteins that spontaneously insert into hydrophobic lipid bilayers. We have used magic-angle spinning solid-state nuclear magnetic resonance spectroscopy to examine the conformational differences between the water-soluble and the membrane-bound states of colicin Ia channel domain, and to study the effect of bound colicin on lipid bilayer structure and dynamics. We detected ¹³C and ¹⁵N isotropic chemical shift differences between the two forms of the protein, which indicate structural changes of the protein due to membrane binding. The Val Cα signal, unambiguously assigned by double-quantum experiments, gave a 0.6 ppm downfield shift in the isotropic position and a 4 ppm reduction in the anisotropic chemical shift span after membrane binding. These suggest that the α-helices in the membrane-bound colicin adopt more ideal helical torsion angles as they spread onto the membrane. Colicin binding significantly reduced the lipid chain order, as manifested by ²H quadrupolar couplings. These results are consistent with the model that colicin Ia channel domain forms an extended helical array at the membrane-water interface upon membrane binding.     

Comparison of the macroscopic and single channel conductance properties of colicin E1 and its COOH-terminal tryptic peptide

A COOH-terminal tryptic fragment (Mr approximately equal to 20,000) of colicin E1 has been proposed to contain the membrane channel-forming domain of the colicin molecule. A comparison is made of the conductance properties of colicin E1 and its COOH-terminal fragment in planar bilayer membranes. The macroscopic and single channel properties of colicin E1 and its COOH-terminal tryptic fragment are very similar, if not indistinguishable, implying that the NH2-terminal, two-thirds of the colicin E1 molecule, does not significantly influence its channel properties. The channel-forming activity of both polypeptides is dependent upon the presence of a membrane potential, negative on the trans side of the membrane. The average single channel conductance of colicin E1 and the COOH-terminal fragment is 20.9 +/- 3.9 and 19.1 +/- 2.9 picosiemens, respectively. The rate at which both proteins form conducting channels increases as the pH is lowered from 7 to 5. Both molecules require negatively charged lipids for activity to be expressed, exhibit the same ion selectivity, and rectify the current to the same extent. Both polypeptides associate irreversibly with the membrane in the absence of voltage, but subsequent formation of conducting channels requires a negative membrane potential.     

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.     

Dynamic properties of the colicin E1 ion channel

Abstract The mechanism of channel formation and action of channel-forming colicins is a paradigm for the study of dynamic aspects of membrane-protein interactions. The following experimental results concerning interaction of the colicin E1 channel domain with target membranes, in vitro and in vivo, are discussed: (1) the nature of the translocation-competent state of the channel-forming domain; (2) unfolding of the colicin channel peptide during in vitro binding and anchoring of the channel to liposome membranes at acidic pH; (3) reversal of channel peptide binding to liposomes by an alkaline-directed pH shift; (4) voltage-driven translocation and gating of the ion channel, discussed in the context of a four-helix model for a monomeric channel; (5) rescue of colicin-treated cells by high levels of external K⁺; (6) trypsin rescue of cells depolarized by the colicin ion channel; and (7) interaction of the channel domain with its immunity protein.     

Lipid-mediated inactivation of colicin E1 channels by calcium ions

Based on the model of a toroidal protein-lipid pore, the effect of calcium ions on colicin E1 channel was predicted. In electrophysiological experiments Ca2+ suppressed the activity of colicin E1 channels in membranes formed of diphytanoylphosphatidylglycerol, whereas no desorption of the protein occurred from the membrane surface. The effect of Ca2+ was not observed on membranes formed of diphytanoylphosphatidylcholine. Single-channel measurements revealed that Ca2+-induced reduction of the colicin-induced current across the negatively charged membrane was due to a decrease in the number of open colicin channels and not changes in their properties. In line with the toroidal model, the effect of Ca2+ on the colicin E1 channel-forming activity is explained by alteration of the membrane lipid curvature caused by electrostatic interaction of Ca2+ with negatively charged lipid head groups.     

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.     

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.     

Insertion intermediates of pore-forming colicins in membrane two-dimensional space

The formation of integral membrane voltage-gated ion channels by the initially soluble C-terminal channel polypeptide (CP) of the pore-forming colicins is a fruitful area for studies on membrane protein import. The dependence of CP import on specific membrane parameters can be better understood using liposomes and planar membranes of defined lipid composition. The membrane surface and interfacial layer provide special conditions for the transition of a pore-forming colicin from the soluble to the integral membrane state. The colicin E1 CP is arranged in the membrane interfacial layer as a conformationally mobile helical array that is extended far more in the two dimensions parallel to the membrane surface than in the third dimension perpendicular to it. The alpha-helical content of CP(E1) increases by approximately 30% upon binding to the membrane. The sequence of kinetically distinguishable events in the CP(E1)-membrane interaction is binding, unfolding to a subtended area of 4200 A(2), helix extension, and insertion, the last three events overlapping in their time course ( approximately 10 s(-1)). The extension into two dimensions and the interaction with the membrane surface may explain the reversible denaturation and refolding of secondary structure that occurs after boiling of the CP-membrane complex. Although DSC showed the presence of helix-helix interactions in the membrane-bound state, the change in secondary structure and the extended surface area argue against a molten-globule intermediate in the CP-membrane interaction. However, the surface-bound state is mobile, as surface conformational mobility is a necessary prerequisite for insertion of CP trans-membrane helices into the bilayer. The requirement for this surface protein mobility, described by "thermal melting" FRET experiments, may provide the explanation for the precipitous decrease in the voltage-gated CP channel formation at high values of surface potential of planar bilayer membranes. Thus, the membrane interfacial layer, with the CP backbone situated near the acyl chain carbonyls, provides a favorable environment for the structure changes necessary for the transition from the soluble to the membrane-inserted state.