Lipid interaction of Pseudomonas aeruginosa exotoxin A. Acid-triggered permeabilization and aggregation of lipid vesicles.

We have investigated the interaction of Pseudomonas exotoxin A with small unilamellar vesicles comprised of different phospholipids as a function of pH, toxin, and lipid concentration. We have found that this toxin induces vesicle permeabilization, as measured by the release of a fluorescent dye. Permeabilization is due to the formation of ion-conductive channels which we have directly observed in planar lipid bilayers. The toxin also produces vesicle aggregation, as indicated by an increase of the turbidity. Aggregation and permeabilization have completely different time course and extent upon toxin dose and lipid composition, thus suggesting that they are two independent events. Both time constants decrease by lowering the pH of the bulk phase or by introducing a negative lipid into the vesicles. Our results indicate that at least three steps are involved in the interaction of Pseudomonas exotoxin A with lipid vesicles. After protonation of one charged group the toxin becomes competent to bind to the surface of the vesicles. Binding is probably initiated by an electrostatic interaction because it is absolutely dependent on the presence of acidic phospholipids. Binding is a prerequisite for the subsequent insertion of the toxin into the lipid bilayer, with a special preference for phosphatidylglycerol-containing membranes, to form ionic channels. At high toxin and vesicle concentrations, bound toxin may also induce aggregation of the vesicles, particularly when phosphatidic acid is present in the lipid mixture. A quenching of the intrinsic tryptophan fluorescence of the protein, which is induced by lowering the pH of the solution, becomes more drastic in the presence of lipid vesicles. However, this further quenching takes so long that it cannot be a prerequisite to either vesicle permeabilization or aggregation. Pseudomonas exotoxin A shares many of these properties with other bacterial toxins like diphtheria and tetanus toxin.     

Pore formation by Staphylococcus aureus alpha-toxin in lipid bilayers

Staphylococcus aureus -toxin forms ionic channels of large size in lipid bilayer membranes. We have developed two methods for studying the mechanism of pore formation. One is based on measurement of the ionic current flowing through a planar lipid membrane after exposure to the toxin; the other is based on measuring the release of the fluorescent complex Tb-Dipicolinic acid from large unilamellar vesicles under similar conditions.Both methods indicate that the pore formation process is complex, showing an initial delay followed by non-linear kinetics. The power dependence of the pore formation rate on the toxin concentration in planar bilayers indicates that an aggregation mechanism underlies the channel assembly. Arrhenius plots, obtained with both techniques, show no deviation from linearity up to 50°C and the derived activation energies are found to be comparable to those for the binding and the lysis of rabbit erythrocytes by the same toxin.The temperature dependence of the conductance induced in planar bilayers by a large number of toxin channels indicates that the pores are filled with aqueous solution. The analysis of single conductance events shows that a heterogeneous population of pores exist and that smaller channels are preferred at low temperature. We attribute this heterogeneity to the existence of pores resulting from the aggregation of different numbers of monomers.     

The Mechanism of a Nuclear Pore Assembly: A Molecular Biophysics View

The basic problem of nuclear pore assembly is the big perinuclear space that must be overcome for nuclear membrane fusion and pore creation. Our investigations of ternary complexes: DNA–PC liposomes–Mg²⁺, and modern conceptions of nuclear pore structure allowed us to introduce a new mechanism of nuclear pore assembly. DNA-induced fusion of liposomes (membrane vesicles) with a single-lipid bilayer or two closely located nuclear membranes is considered. After such fusion on the lipid bilayer surface, traces of a complex of ssDNA with lipids were revealed. At fusion of two identical small liposomes (membrane vesicles) <100 nm in diameter, a “big” liposome (vesicle) with ssDNA on the vesicle equator is formed. ssDNA occurrence on liposome surface gives a biphasic character to the fusion kinetics. The “big” membrane vesicle surrounded by ssDNA is the base of nuclear pore assembly. Its contact with the nuclear envelope leads to fast fusion of half of the vesicles with one nuclear membrane; then ensues a fusion delay when ssDNA reaches the membrane. The next step is to turn inside out the second vesicle half and its fusion to other nuclear membrane. A hole is formed between the two membranes, and nucleoporins begin pore complex assembly around the ssDNA. The surface tension of vesicles and nuclear membranes along with the kinetic energy of a liquid inside a vesicle play the main roles in this process. Special cases of nuclear pore formation are considered: pore formation on both nuclear envelope sides, the difference of pores formed in various cell-cycle phases and linear nuclear pore clusters.     

Kinetics of melittin induced pore formation in the membrane of lipid vesicles.

We have investigated the permeabilization of POPC unilamellar vesicle bilayers upon the addition of melittin. This process was measured in an early time range of a few minutes by means of monitoring the release of an entrapped marker, the self-quenching fluorescent dye carboxyfluorescein. Pore formation is indicated by an apparent 'all-or-none' efflux out of individual vesicles and a higher than linear dependence on melittin concentration. Applying a recently developed evaluation procedure, the data are readily converted into the gross number of pores per vesicle formed within the elapsed measuring time t. The results can be generally described in terms of a fast initial rate of pore formation that slows down to a much lower value after a period of about 1 to 2 minutes, following a single exponential time course. The three rate parameters involved are shown to be power functions of the concentration of melittin that is actually associated with the vesicle membrane. These findings are in excellent quantitative agreement with a proposed scheme of reaction steps where the formation of lipid associated peptide dimers becomes rate determining once an initial fast deposit is exhausted.     

Visualization of Membrane Loss during the Shrinkage of Giant Vesicles under Electropulsation

We study the effect of permeabilizing electric fields applied to two different types of giant unilamellar vesicles, the first formed from EggPC lipids and the second formed from DOPC lipids. Experiments on vesicles of both lipid types show a decrease in vesicle radius, which is interpreted as being due to lipid loss during the permeabilization process. We show that the decrease in size can be qualitatively explained as a loss of lipid area, which is proportional to the area of the vesicle that is permeabilized. Three possible modes of membrane loss were directly observed: pore formation, vesicle formation, and tubule formation.     

Assembly of the nuclear pore: biochemically distinct steps revealed with NEM, GTP gamma S, and BAPTA

A key event in nuclear formation is the assembly of functional nuclear pores. We have used a nuclear reconstitution system derived from Xenopus eggs to examine the process of nuclear pore assembly in vitro. With this system, we have identified three reagents which interfere with nuclear pore assembly, NEM, GTP gamma S, and the Ca++ chelator, BAPTA. These reagents have allowed us to determine that the assembly of a nuclear pore requires the prior assembly of a double nuclear membrane. Inhibition of nuclear vesicle fusion by pretreatment of the membrane vesicle fraction with NEM blocks pore complex assembly. In contrast, NEM treatment of already fused double nuclear membranes does not block pore assembly. This indicates that NEM inhibits a single step in pore assembly--the initial fusion of vesicles required to form a double nuclear membrane. The presence of GTP gamma S blocks pore assembly at two distinct steps, first by preventing fusion between nuclear vesicles, and second by blocking a step in pore assembly that occurs on already fused double nuclear membranes. Interestingly, when the Ca2+ chelator BAPTA is added to a nuclear assembly reaction, it only transiently blocks nuclear vesicle fusion, but completely blocks nuclear pore assembly. This results in the formation of a nucleus surrounded by a double nuclear membrane, but devoid of nuclear pores. To order the positions at which GTP gamma S and BAPTA interfere with pore assembly, a novel anchored nuclear assembly assay was developed. This assay revealed that the BAPTA-sensitive step in pore assembly occurs after the second GTP gamma S-sensitive step. Thus, through use of an in vitro nuclear reconstitution system, it has been possible to biochemically define and order multiple steps in nuclear pore assembly.     

All-or-none versus graded: single-vesicle analysis reveals lipid composition effects on membrane permeabilization

We report a single-vesicle approach to compare the all-or-none and graded mechanisms of lipid bilayer permeabilization by CpreTM and NpreTM, two peptides derived from the membrane-proximal external region of the HIV fusion glycoprotein gp41subunit. According to bulk requenching assays, these peptides permeabilize large unilamellar vesicles via all-or-none and graded mechanisms, respectively. Visualization of the process using giant unilamellar vesicles shows that the permeabilization of individual liposomes by these two peptides differs in kinetics, degree of dye filling, and stability of the permeabilized state. All-or-none permeabilization by CpreTM is characterized by fast and total filling of the individual vesicles. This process is usually accompanied by the formation of stably open pores, as judged from the capacity of the vesicles to incorporate a second dye added after several hours. In contrast, graded permeabilization by NpreTM is transient and exhibits slower kinetics, which leads to partial filling of the individual liposomes. Of importance, quantitative analysis of vesicle population distribution allowed the identification of mixed mechanisms of membrane permeabilization and the assessment of cholesterol effects. Specifically, the presence of this viral envelope lipid increased the stability of the permeating structures, which may have implications for the fusogenic activity of gp41.     

Interaction of tetanus toxin with lipid vesicles. Effects of pH, surface charge, and transmembrane potential on the kinetics of channel formation.

We investigated the interaction of tetanus toxin with small unilamellar vesicles composed of different phospholipids as a function of pH, toxin concentration, temperature, and ionic strength of the solution. Tetanus toxin increased the permeability of the vesicles to fluorescent markers of molecular weight up to 700. The time course of the permeabilization was described as the sum of two exponential components of which the faster accounts for more than 70% of the total effect. Both time constants decreased when the pH of the solution was lowered and when vesicles contained negative lipids. These results can be explained in terms of a phenomenological model based on reaction rate theory. The model assumes that tetanus toxin, after equilibrating with the local pH existing at the surface of the vesicles, inserts into the lipid bilayer forming an ionic channel through which solutes can diffuse. Trigger event for the insertion of the toxin is the protonation, and consequent neutralization of one charged group which makes the molecule more hydrophobic. The intrinsic pK of this group was found to be 3.4 +/- 0.2, suggesting that it may be a carboxyl group. Since the toxin equilibrates with the local pH, the enhancing effect of acidic phospholipids is merely explained by the creation of a negative surface potential which increases the local proton concentration. This was confirmed by the inhibitory effect of high Na+ concentration which reduced the surface charge by screening and specific binding. We found still small differences between the lipids tested and the following order of sensitivity to the action of the toxin: phosphatidylinositol greater than phosphatidylserine greater than phosphatidylcholine approximately cholesterol. The activation energy for the two time constants was found to be 19.8 and 14.8 kcal/mol, fast and slow component, respectively, i.e., slightly larger than that for pure diffusion through the bilayer. The permeabilization induced by tetanus toxin is a voltage-dependent process because vesicles bearing an inner negative potential were depolarized very quickly whereas those bearing an inner positive voltage were barely depolarized at all.     

Synergistic pore formation by type III toxin translocators of Pseudomonas aeruginosa

Type III secretion/translocation systems are essential actors in the pathogenicity of Gram-negative bacteria. The injection of bacterial toxins across the host cell plasma membranes is presumably accomplished by a proteinaceous structure, the translocon. In vitro, Pseudomonas aeruginosa translocators PopB and PopD form ringlike structures observed by electron microscopy. We demonstrate here that PopB and PopD are functionally active and sufficient to form pores in lipid vesicles. Furthermore, the two translocators act in synergy to promote membrane permeabilization. The size-based selectivity observed for the passage of solutes indicates that the membrane permeabilization is due to the formation of size-defined pores. Our results provide also new insights into the mechanism of translocon pore formation that may occur during the passage of toxins from the bacterium into the cell. While proteins bind to lipid vesicles equally at any pH, the kinetics of membrane permeabilization accelerate progressively with decreasing pH values. Electrostatic interactions and the presence of anionic lipids were found to be crucial for pore formation whereas cholesterol did not appear to play a significant role in functional translocon formation.     

Fluctuations and the Rate-Limiting Step of Peptide-Induced Membrane Leakage

Peptide-induced vesicle leakage is a common experimental test for the membrane-perturbing activity of antimicrobial peptides. The leakage kinetics is usually very slow, requiring minutes to hours for complete release of vesicle contents, and exhibits a biphasic behavior. We report here that, in the case of the peptaibol trichogin GA IV, all processes involved in peptide-membrane interaction, such as peptide-membrane association, peptide aggregation, and peptide translocation, take place on a timescale much shorter than the leakage kinetics. On the basis of these findings, we propose a stochastic model in which the leakage kinetics is determined by the discrete nature of a vesicle suspension: peptides are continuously exchanging among vesicles, producing significant fluctuations over time in the number of peptide molecules bound to each vesicle, and in the formation of pores. According to this model, the fast initial leakage is caused by vesicles that contain at least one pore after the peptides are randomly distributed among the liposomes, whereas the slower release is associated with the time needed to occasionally reach in an intact vesicle the critical number of bound peptides necessary for pore formation. Fluctuations due to peptide exchange among vesicles therefore represent the rate-limiting step of such a slow mechanism.     

Capture of AT-rich chromatin by ELYS recruits POM121 and NDC1 to initiate nuclear pore assembly

Assembly of the nuclear pore, gateway to the genome, from its component subunits is a complex process. In higher eukaryotes, nuclear pore assembly begins with the binding of ELYS/MEL-28 to chromatin and recruitment of the large critical Nup107-160 pore subunit. The choreography of steps that follow is largely speculative. Here, we set out to molecularly define early steps in nuclear pore assembly, beginning with chromatin binding. Point mutation analysis indicates that pore assembly is exquisitely sensitive to the change of only two amino acids in the AT-hook motif of ELYS. The dependence on AT-rich chromatin for ELYS binding is borne out by the use of two DNA-binding antibiotics. AT-binding Distamycin A largely blocks nuclear pore assembly, whereas GC-binding Chromomycin A(3) does not. Next, we find that recruitment of vesicles containing the key integral membrane pore proteins POM121 and NDC1 to the forming nucleus is dependent on chromatin-bound ELYS/Nup107-160 complex, whereas recruitment of gp210 vesicles is not. Indeed, we reveal an interaction between the cytoplasmic domain of POM121 and the Nup107-160 complex. Our data thus suggest an order for nuclear pore assembly of 1) AT-rich chromatin sites, 2) ELYS, 3) the Nup107-160 complex, and 4) POM121- and NDC1-containing membrane vesicles and/or sheets, followed by (5) assembly of the bulk of the remaining soluble pore subunits.     

Effects of lipid composition on membrane permeabilization by sticholysin I and II, two cytolysins of the sea anemone Stichodactyla helianthus

Sticholysin I and II (St I and St II), two basic cytolysins purified from the Caribbean sea anemone Stichodactyla helianthus, efficiently permeabilize lipid vesicles by forming pores in their membranes. A general characteristic of these toxins is their preference for membranes containing sphingomyelin (SM). As a consequence, vesicles formed by equimolar mixtures of SM with phosphatidylcholine (PC) are very good targets for St I and II. To better characterize the lipid dependence of the cytolysin-membrane interaction, we have now evaluated the effect of including different lipids in the composition of the vesicles. We observed that at low doses of either St I or St II vesicles composed of SM and phosphatidic acid (PA) were permeabilized faster and to a higher extent than vesicles of PC and SM. As in the case of PC/SM mixtures, permeabilization was optimal when the molar ratio of PA/SM was ~1. The preference for membranes containing PA was confirmed by inhibition experiments in which the hemolytic activity of St I was diminished by pre-incubation with vesicles of different composition. The inclusion of even small proportions of PA into PC/SM LUVs led to a marked increase in calcein release caused by both St I and St II, reaching maximal effect at ~5 mol % of PA. Inclusion of other negatively charged lipids (phosphatidylserine (PS), phosphatidylglycerol (PG), phosphatidylinositol (PI), or cardiolipin (CL)), all at 5 mol %, also elicited an increase in calcein release, the potency being in the order CL approximately PA > PG approximately PI approximately PS. However, some boosting effect was also obtained, including the zwitterionic lipid phosphatidylethanolamine (PE) or even, albeit to a lesser extent, the positively charged lipid stearylamine (SA). This indicated that the effect was not mediated by electrostatic interactions between the cytolysin and the negative surface of the vesicles. In fact, increasing the ionic strength of the medium had only a small inhibitory effect on the interaction, but this was actually larger with uncharged vesicles than with negatively charged vesicles. A study of the fluidity of the different vesicles, probed by the environment-sensitive fluorescent dye diphenylhexatriene (DPH), showed that toxin activity was also not correlated to the average membrane fluidity. It is suggested that the insertion of the toxin channel could imply the formation in the bilayer of a nonlamellar structure, a toroidal lipid pore. In this case, the presence of lipids favoring a nonlamellar phase, in particular PA and CL, strong inducers of negative curvature in the bilayer, could help in the formation of the pore. This possibility is confirmed by the fact that the formation of toxin pores strongly promotes the rate of transbilayer movement of lipid molecules, which indicates local disruption of the lamellar structure.     

A theory of osmotic lysis of lipid vesicles

Osmotic lysis of vesicles is shown to begin when the membrane expansion due to osmotic pressure exceeds its critical value, delta S, at which a membrane ruptures to form a pore. The dependence of delta S on the vesicle radius and respective osmotic pressures are obtained. It is found that osmotic pressure necessary for small (100 A) vesicles to rupture should exceed 30 atm, for large (10 000 A) vesicles it being as small as 10(-3) atm. In the case of large (greater than or approximately 1000 A) vesicles the value of relative expansion of the membrane at which its rupture occurs in a reasonable time only depends slightly on the vesicle radius. For instance, for 10 000 A vesicles it amounts to 3%. The tension of membrane rupture is about 8 dyn/cm for large vesicles. Membrane tension, although it decreases considerably as a result of rupture and pore formation, does not vanish completely. It supports the residual intravesicular pressure causing the efflux of vesicle (cell) contents. Simultaneously, osmotic influx of water through the membrane occurs that results in either complete rupture of the membrane with the efflux of the whole of the contents, or its gradual washout in either of two, quasi-steady or pulse-wise regimes. In the first case a pore is steadily open, whereas in the second case it alternately opens and closes, ejecting about 5% of internal solution each time. Lysis kinetics is analyzed. Pulse-wise regime of lysis is shown to be the most likely one.     

Influence of the biophysical and biochemical environment on the kinetics of pore formation by Cry toxins

The effect of Bacillus thuringiensis toxins on the permeability of the luminal membrane of Manduca sexta midgut columnar epithelial cells is strongly influenced by several biophysical and biochemical factors, including pH, ionic strength, and divalent cations, suggesting an important role for electrostatic interactions. The influence of these factors can differ greatly, however, depending on the toxin being studied, even for closely related toxins such as Cry1Ac and Cry1Ca. In the present study, the possibility of using temperature changes as a tool for controlling the rate and extent of pore formation in midgut brush border membrane vesicles was evaluated. Lowering temperature gradually decreased the rate of pore formation, but had little effect on the permeability of vesicles previously incubated with toxin at room temperature. The formation of new pores, following incubation of the vesicles with toxin, could thus be almost abolished by rapidly cooling the vesicles to 2 degrees C. Using this approach, changes in the rate of pore formation could be more easily distinguished from alterations in the properties of the pores formed, thus allowing a more detailed analysis of the kinetics and mechanism of pore formation.     

Detergent-resistant membranes are platforms for actinoporin pore-forming activity on intact cells

Sticholysin II is a pore-forming toxin produced by the sea anemone Stichodactyla helianthus. We studied its cytolytic activity on COS-7 cells. Fluorescence spectroscopy and flow cytometry revealed that the toxin permeabilizes cells to propidium cations in a dose-dependent and time-dependent manner. This permeabilization is impaired by preincubation of cells with cyclodextrin. Isolation of detergent-resistant cellular membranes showed that sticholysin II colocalizes with caveolin-1 in fractions corresponding to raft-like domains. The interaction of sticholysin II with such domains is only lipid dependent as it also occurs in the absence of any other membrane-associated protein. Toxin binding to raft-like lipid vesicles inhibited cell permeabilization. The results suggest that sticholysin II promotes pore formation in COS-7 cells through interaction with membrane domains which behave like cellular rafts.     

Kinetics of pore formation by the Bacillus thuringiensis toxin Cry1Ac

After binding to specific receptors, Cry toxins form pores in the midgut apical membrane of susceptible insects. The receptors could form part of the pore structure or simply catalyze pore formation and consequently be recycled. To discriminate between these possibilities, the kinetics of pore formation in brush border membrane vesicles isolated from Manduca sexta was studied with an osmotic swelling assay. Pore formation, as deduced from changes in membrane permeability induced by Cry1Ac during a 60-min incubation period, was strongly dose-dependent, but rapidly reached a maximum as toxin concentration was increased. Following exposure of the vesicles to the toxin, the osmotic swelling rate reached a maximum shortly after a delay period. Under these conditions, at relatively high toxin concentrations, the maximal osmotic swelling rate increased linearly with toxin concentration. When vesicles were incubated for a short time with the toxin and then rapidly cooled to prevent the formation of new pores before and during the osmotic swelling experiment, a plateau in the rate of pore formation was observed as toxin concentration was increased. Taken together, these results suggest that the receptors do not act as simple catalysts of pore formation, but remain associated with the pores once they are formed.     

Kinetics of pore formation by the Bacillus thuringiensis toxin Cry1Ac

After binding to specific receptors, Cry toxins form pores in the midgut apical membrane of susceptible insects. The receptors could form part of the pore structure or simply catalyze pore formation and consequently be recycled. To discriminate between these possibilities, the kinetics of pore formation in brush border membrane vesicles isolated from Manduca sexta was studied with an osmotic swelling assay. Pore formation, as deduced from changes in membrane permeability induced by Cry1Ac during a 60-min incubation period, was strongly dose-dependent, but rapidly reached a maximum as toxin concentration was increased. Following exposure of the vesicles to the toxin, the osmotic swelling rate reached a maximum shortly after a delay period. Under these conditions, at relatively high toxin concentrations, the maximal osmotic swelling rate increased linearly with toxin concentration. When vesicles were incubated for a short time with the toxin and then rapidly cooled to prevent the formation of new pores before and during the osmotic swelling experiment, a plateau in the rate of pore formation was observed as toxin concentration was increased. Taken together, these results suggest that the receptors do not act as simple catalysts of pore formation, but remain associated with the pores once they are formed.     

Membrane Bending Energy and Fusion Pore Kinetics in Ca-Triggered Exocytosis

A fusion pore composed of lipid is an obligatory kinetic intermediate of membrane fusion, and its formation requires energy to bend membranes into highly curved shapes. The energetics of such deformations in viral fusion is well established, but the role of membrane bending in Ca²⁺-triggered exocytosis remains largely untested. Amperometry recording showed that during exocytosis in chromaffin and PC12 cells, fusion pores formed by smaller vesicles dilated more rapidly than fusion pores formed by larger vesicles. The logarithm of 1/(fusion pore lifetime) varied linearly with vesicle curvature. The vesicle size dependence of fusion pore lifetime quantitatively accounted for the nonexponential fusion pore lifetime distribution. Experimentally manipulating vesicle size failed to alter the size dependence of fusion pore lifetime. Manipulations of membrane spontaneous curvature altered this dependence, and applying the curvature perturbants to the opposite side of the membrane reversed their effects. These effects of curvature perturbants were opposite to those seen in viral fusion. These results indicate that during Ca²⁺-triggered exocytosis membrane bending opposes fusion pore dilation rather than fusion pore formation. Ca²⁺-triggered exocytosis begins with a proteinaceous fusion pore with less stressed membrane, and becomes lipidic as it dilates, bending membrane into a highly curved shape.     

Mechanisms of leakage

Abstract

Two mechanisms of leakage from liposomes are discussed, (i) Cations such as Ca²⁺ induce graded release whose rate depends mainly on vesicle collisions and is associated in the case of several acidic phospholipids with fusion events. A certain degree of leakage also occurs in between collisions. Consequently, the leakage per fusion is reduced at larger lipid and Ca concentrations, (n) Certain peptides induce leakage by pore formation, which shows selectivity to the size of the entrapped molecules and occurs by an all or none mechanism; vesicles either leak or retain all of their contents. A model for final extents and kinetics of leakage due to pore forming peptides is described. This model assumes that pore forming peptides become incorporated into the vesicle bilayer and aggregate to form a pore. Recent developments in the model enable considerations of a reversible or irreversible surface aggregation of peptides. Results of final extents and kinetics of leakage induced by pore forming peptides can be well explained and predicted by this formalism. Studies demonstrate that Ca can play a dual role in affecting leakage. A case is presented where Ca ⁺ inhibits and can even arrest pore formation by a peptide, while promoting vesicle fusion. Conversely, formation of pore structures by a peptide can inhibit vesicle fusion.