Channels formed by colicin E1 in planar lipid bilayers are large and exhibit pH-dependent ion selectivity

Summary The E1 subgroup (E1, A, Ib, etc.) of antibacterial toxins called colicins are known to form voltage-dependent channels in planar lipid bilayers. The genes for colicins E1, A and Ib have been cloned and sequenced, making these channels interesting models for the widespread phenomenon of voltage dependence in cellular channels. In this paper we investigate ion selectivity and channel size—properties relevant to model building. Our major finding is that the colicin E1 channel is large, having a diameter ofat least 8 Å at its narrowest point. We established this from measurements of reversal potentials for gradients formed by salts of large cations or large anions. In so doing, we exploited the fact that the colicin channel is permeable to both cations and anions, and its relative selectivity to them is a functions and anions, and its relative selectivity to them is a function of pH. The channel is anion selective (Cl^– over K⁺) in neutral membranes, and the degree of selectivity is highly dependent on pH. In negatively charged membranes, it becomes cation selective at pH's higher than about 5. Experiments with pH gradients cross the membrane suggest that titratable groups both within the channel lumen and near the channel ends affect the selectivity. Individual E1 channels have more than one open conductance state, all displaying comparable ion selectivity. Colicins A and Ib also exhibit pH-dependent ion selectivity, and appear to have even larger lumens than E1.     

Gating processes of channels induced by colicin A,its C-terminal fragment and colicin E1 in planar lipid bilayers

The dependence on pH and membrane potential of the pore formed by colicin A and its C-terminal 20 kDa fragment has been measured using planar lipid bilayers. The single channel conductance of the pore formed by both colicin A and the fragment increases with pH with an apparent pK of 6.0. At pH 5.0 the gating by membrane potential of the channels formed by either colicin A or its fragment is identical. At the same pH, quite similar pore properties were found when using the related bacteriocin, colicin E₁. In agreement with previous studies, these data indicate that the protein structure containing the lumen of the pore resides in the 20 kDa C-terminal part of the colicin A and favours the recently proposed model, based on protein sequence analysis, which proposes that colicin A, E₁ and I_B C-terminal domains are folded in the same three-dimensional structure. However, it is also shown that colicin A and not its C-terminal fragment undergoes a pH dependent transition between an acidic and a basic form of the pore with an apparent pK of 5.3. The two forms of the pore differ by their gating charge but not by the channel size. These results suggest that there is a pH dependent association between the C-terminal domain carrying the lumen of the pore and another domain of the molecule which affect the pore sensitivity to membrane potential.     

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.     

Membrane binding of the colicin E1 channel: activity requires an electrostatic interaction of intermediate magnitude.

In vitro channel activity of the C-terminal colicin E1 channel polypeptide under conditions of variable electrostatic interaction with synthetic lipid membranes showed distinct maxima with respect to pH and membrane surface potential. The membrane binding energy was determined from fluorescence quenching of the intrinsic tryptophans of the channel polypeptide by liposomes containing N-trinitrophenyl-phosphatidylethanolamine. Maximum in vitro colicin channel activity correlated with an intermediate magnitude of the electrostatic interaction. For conditions associated with maximum activity (40% anionic lipid, I = 0.12 M, pH 4.0), the free energy of binding was delta G approximately -9 kcal/mol, with nonelectrostatic and electrostatic components, delta Gnel approximately -5 kcal/mol and delta Gel approximately -4 kcal/mol, and an effective binding charge of +7 at pH 4.0. Binding of the channel polypeptide to negative membranes at pH 8 is minimal, whereas initial binding at pH 4 followed by a shift to pH 8 causes only 3-10% reversal of binding, implying that it is kinetically trapped, probably by a hydrophobic interaction. It was inferred that membrane binding and insertion involves an initial electrostatic interaction responsible for concentration and binding to the membrane surface. This is followed by insertion into the bilayer driven by hydrophobic forces, which are countered in the case of excessive electrostatic binding.     

A Novel Approach to Study the Geometry of the Water Lumen of Ion Channels: Colicin Ia Channels in Planar Lipid Bilayers

This paper describes a new approach to evaluate the inner structure (including a main constriction and its localization) of the water lumen of an ion channel. The method is based on the determination of channel filling by different nonelectrolyte molecules through each side of an ion channel. The method has two characteristic features that make its use attractive: (i) the possibility to ascertain the existence, localization and size of a narrow part inside an ion channel water lumen and (ii) the chances to determine the maximal size of both entrances of an ion channel and to obtain additional information about the geometry of its water lumen at the same time. Determinations were made on colicin Ia ion channels inserted into planar lipid bilayers. This channel was chosen because there is an apparent contradiction between its low single channel conductance and the large diameter of its water lumen. Our results show that the water lumen of the colicin Ia channel has a funnel-like structure with a small trans-entrance, with a diameter of about 1.0 nm, and a large cis-entrance, with a diameter of approximately 1.8 nm. A constriction with a diameter of approximately 0.7 nm is shown to be located close to the trans-entrance of the channel. The method can also be applied to patch clamp studies of single ion channels. Received: 20 February 1997/Revised: 19 August 1997     

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.     

Ion selectivity of colicin E1: III. Anion permeability

The antibiotic protein colicin E1 forms ion channels in planar lipid bilayers that are capable of conducting monovalent organic cations having mean diameters of at least 9 Å. Polyvalent organic cations appear to be completely impermeant, regardless of size. All permeant ions, whether large or small, positively or negatively charged, are conducted by this channel at very slow rates. We have examined the permeability of colicin E1 channels to anionic probes having a variety of sizes, shapes, and charge distributions. In contrast to the behavior of cations, polyvalent as well as monovalent organic anions were found to permeate the colicin E1 channel. Inorganic sulfate was able to permeate the channel only when the pH was 4 or less, conditions under which the colicin E1 protein is predominantly in an anion-preferring conformational state. The less selective state(s) of the colicin E1 channel, observed when the pH was 5 or greater, was not permeable to inorganic sulfate. The sulfate salt of the impermeant cation Bis-T6 (N,N,N,N-tetramethyl-1,6-hexanediamine) had no effect on the single channel conductance of colicin E1 channels exposed to solutions containing 1 m NaCl at pH 5. The complete lack of blocking activity by either of these two impermeant ions indicates that both are excluded from the channel lumen. These results are consistent with our hypothesis that there is but a single location in the lumen of the colicin E1 channel where positively charged groups can be effectively hydrated. This site may coincide with the location of the energetic barrier which impedes the movement of anions.The authors wish to thank Dr. F.S. Cohen for making available unpublished data and for helpful comments. This work was supported by National Institutes of Health grant GM 37396 and by the Howard Hughes Medical Institute Undergraduate Biological Sciences Education Initiative (E.R.K.)     

A single tryptic fragment of colicin E1 can form an ion channel: stoichiometry confirms kinetics.

The molecularity of the ion channel formed by peptide fragments of colicin has taken on particular significance since the length of the active peptide has been shown to be less than 90 amino acids and the lumen size at least 8 A. Cell survival experiments show that killing by colicin obeys single-hit statistics, and ion leakage rates from phospholipid vesicles are first order in colicin concentration. However, interpretation in molecular terms is generally complicated by the requirement of large numbers of colicin molecules per cell or vesicle. We have measured the discharge of potential across membranes of small phospholipid vesicles by following the changes in binding of potential sensitive spin labeled phosphonium ions as a function of the number of colicin fragments added. Because of the sensitivity of the method, it was possible to reliably investigate the effect of colicin in a range where there was no more than 0.2 colicins per vesicle. The quantitative results of these experiments yield a direct molecular stoichiometry and demonstrate that one C-terminal fragment of the colicin molecule per one vesicle is sufficient to induce a rapid ion flux in these vesicles. In addition, the experiments confirm earlier findings that the colicin fragments do not migrate from one vesicle to another at pH 4.5. Similar results are obtained with large unilamellar vesicles.     

Membrane topography of ColE1 gene products: the hydrophobic anchor of the colicin E1 channel is a helical hairpin.

The paucity of crystallographic data on the structure of intrinsic membrane proteins necessitates the development of additional techniques to probe their structures. The colicin E1 ion channel domain contains one prominent hydrophobic region near its COOH terminus that has been proposed to be an anchor for the assembly of the channel. Saturation site-directed mutagenesis of the hydrophobic anchor region of the colicin E1 ion channel was used to probe whether it spanned the bilayer once or twice. A nonpolar amino acid was replaced by a charged residue in 29 mutations made at 26 positions in the channel domain. Substitution of the charged amino acid at all positions except those in the center of the hydrophobic region and the periphery of the hydrophobic region caused a large decrease in the cytotoxicity of the purified mutant colicin E1 protein. This result implies that the hydrophobic domain spans the membrane bilayer twice in a helical hairpin loop, with the center of this domain residing in an aqueous or polar phase. The lengths of the trans-membrane helices appear to be approximately 18 and 16 residues. The absence of significant changes in ion selectivity in five of nine mutants indicated that these mutations did not cause a large change in the channel structure. The ion selectivity changes in four mutants and those previously documented for the flanking Lys residues imply that the hydrophobic hairpin is part of the channel lumen. Water may "abhor" the hydrophobic side of the channel, explaining the small effects of residue charge changes on ion selectivity.     

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.     

On the nature of the unfolded intermediate in the in vitro transition of the colicin E1 channel domain from the aqueous to the membrane phase.

The transition of the colicin E1 channel polypeptide from a water-soluble to membrane-bound state occurs in vitro at acid pH values that are associated with an unfolded channel structure whose properties qualitatively resemble those of a "molten globule," or "compact unfolded," intermediate state. The role of such a state for activity was tested by comparing the pH dependence of channel-induced solute efflux and the amplitude of the near-UV CD spectrum. The requirement of a partly unfolded state for activity was shown by the coincidence of the onset of channel activity measured for 4 different lipid compositions with the decrease in near-UV CD amplitude as a function of pH. Tertiary constraints on the 3 tryptophans of the colicin channel, assayed by the amplitude of the near-UV CD spectrum, are retained over the pH range 3-4 where channel activity could be measured and, as well, at pH 2. In addition, the tryptophan fluorescence emission spectrum is virtually unchanged over the pH range 2-6. The temperature independence of the near-UV spectrum at pH 3-6 up to 70 degrees C implies that the colicin E1 channel polypeptide is more stable than that of colicin A. A transition between 53 and 58 degrees C in the amplitude of the near-UV CD is consistent with preservation of part of the hydrophobic core in a destabilized state at pH 2. Thus, the unfolded state associated with colicin activity at acidic pH has the properties of a "compact unfolded" state, having some, but not all of the properties of a "molten globule."(ABSTRACT TRUNCATED AT 250 WORDS)     

Speculations on the evolution of ion transport mechanisms.

Primate cells evolved a plasma membrane to restrict the loss of important molecules. The osmotic problems that then arose were solved in one of several ways. Of major importance was the evolution of specific ion pumps, to actively extrude those salts whose inward diffusion would have led to swelling and lysis. In addition, these pumps allowed the cell to store energy in the form of ion gradients across the membrane. Thus, even in the earliest stages, the evolution of ion transport systems coincided with the development of mechanisms which catalyzes the energy transformations. It is postulated that an "ATP"-driven proton pump was one of the first ion transport systems. Such a proton pump would extrude hydrogen ions from the cell, establishing both a transmembrane pH gradient (alkaline inside) and a membrane potential (negative inside). This difference in electrochemical potential for protons (the proton-motive force) could then drive a variety of essential membrane functions, such as the active transport of ions and nutrients. A second major advance was the evolution of an ion transport system that converted light energy into a form which could be used by the cell. The modern model for this is the "purple membrane" of Halobacterium halobium, which catalyzes the extrusion of protons after the capture of light. The protonmotive force generated by such a light-driven proton pump could then power net synthesis of ATP by a reversal of the ATP-driven proton pump. A third important evolutionary step associated with ion transport was the development of a system to harness energy released by biological oxidations. Again, the solution of this problem was to conserve energy as a protonmotive force by coupling the activity of a respiratory chain to the extrusion of protons. Finally, with the development of animal cells a more careful regulation of internal and external pH was required. Thus, an ATP-driven Na+-K+ pump replaced the proton-translocating ATPase as the major ion pump found in plasma membranes.     

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.     

Colicin E1 in planar lipid bilayers

The channel formed by the C-terminal domain of colicin E1 in planar lipid bilayers has proven to be more complex than one might have guessed for such a simple system. The protein undergoes a pH-dependent rearrangement which transforms it from a water soluble form to a much different membrane bound form. There are at least two bound states which don't form a channel. The process by which the channel opens and closes is regulated by the pH and the transmembrane voltage. The voltage is probably sensed by at least 3 (and more likely 4 or more) lysine residues which must be driven through the field to open the channel. The process appears to be hindered by particular carboxyl groups when they are in the unprotonated state. The open channel has several substates and several superstates. Very large positive voltage catalyzes a transition of the open channel to an inactivated state, and may be able to drive the channel-forming region of the protein across the membrane. Little is known about the structure of any of these states, but the open channel is large enough to allow NAD to traverse the membrane and appears to be formed by one colicin molecule. This single polypeptide mimics many of the properties found in channels of mammalian cell membranes, but it may prove more relevant as a model for the transport of proteins across membranes. The comparative ease with which the protein can be manipulated chemically and genetically, along with the complexity of its behavior, promises to keep several laboratories busy for some time.     

Lipid dependence of the channel properties of a colicin E1-lipid toroidal pore

Colicin E1 belongs to a group of bacteriocins whose cytotoxicity toward Escherichia coli is exerted through formation of ion channels that depolarize the cytoplasmic membrane. The lipid dependence of colicin single-channel conductance demonstrated intimate involvement of lipid in the structure of this channel. The colicin formed "small" conductance 60-picosiemens (pS) channels, with properties similar to those previously characterized, in 1,2-dieicosenoyl-sn-glycero-3-phosphocholine (C20) or thinner membranes, whereas it formed a novel "large" conductance 600-pS state in thicker 1,2-dierucoyl-sn-glycero-3-phosphocholine (C22) bilayers. Both channel states were anion-selective and voltage-gated and displayed a requirement for acidic pH. Lipids having negative spontaneous curvature inhibited the formation of both channels but increased the ratio of open 600 pS to 60 pS conductance states. Different diameters of small and large channels, 12 and 16 A, were determined from the dependence of single-channel conductance on the size of nonelectrolyte solute probes. Colicin-induced lipid "flip-flop" and the decrease in anion selectivity of the channel in the presence of negatively charged lipids implied a significant contribution of lipid to the structure of the channel, most readily described as toroidal organization of lipid and protein to form the channel pore.     

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.     

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.     

The pore-forming domain of colicin A fused to a signal peptide: a tool for studying pore-formation and inhibition

Pore-forming colicins are plasmid-encoded bacteriocins that kill Escherichia coli and closely related bacteria. They bind to receptors in the outer membrane and are translocated across the cell envelope to the inner membrane where they form voltage-dependent ion-channels. Colicins are composed of three domains, with the C-terminal domain responsible for pore-formation. Isolated C-terminal pore-forming domains produced in the cytoplasm of E. coli are inactive due to the polarity of the transmembrane electrochemical potential, which is the opposite of that required. However, 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 E. coli from the periplasmic side, forming a functional channel. Sp-pfColA is specifically inhibited by the colicin A immunity protein (Cai). This construct has been used to investigate colicin A channel formation in vivo and to characterise the interaction of pfColA with Cai within the inner membrane. These points will be developed further in this review.     

Studies on colicin B translocation: FepA is gated by TonB

Colicin B is a 55 kDa dumbbell-shaped protein toxin that uses the TonB system (outer membrane transporter, FepA, and three cytoplasmic membrane proteins TonB/ExbB/ExbD) to enter and kill Escherichia coli. FepA is a 22-stranded beta-barrel with its lumen filled by an amino-terminal globular domain containing an N-terminal semiconserved region, known as the TonB box, to which TonB binds. To investigate the mechanism of colicin B translocation across the outer membrane, we engineered cysteine (Cys) substitutions in the globular domain of FepA. Colicin B caused increased exposure to biotin maleimide labelling of all Cys substitutions, but to different degrees, with TonB as well as the FepA TonB box required for all increases. Because of the large increases in exposure for Cys residues from T13 to T51, we conclude that colicin B is translocated through the lumen of FepA, rather than along the lipid-barrel interface or through another protein. Part of the FepA globular domain (residues V91-V142) proved relatively refractory to labelling, indicating either that the relevant Cys residues were sequestered by an unknown protein or that a significant portion of the FepA globular domain remained inside the barrel, requiring concomitant conformational rearrangement of colicin B during its translocation. Unexpectedly, TonB was also required for colicin-induced exposure of the FepA TonB box, suggesting that TonB binds FepA at a different site prior to interaction with the TonB box.     

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.